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Astron. Astrophys. 360, 447-456 (2000) 1. IntroductionBarred galaxies constitute a major fraction of all disc galaxies classified in the optical, more than 50% including strong bars and intermediate morphologies (Sellwood & Wilkinson 1993). This fraction increases when also near-infrared images are used for classification, thus underlining the importance for the general understanding of the evolution of galaxies. The non-axisymmetric potential has a strong impact on the gas dynamics and the star formation in barred systems. Observations reveal a correlation between the radial abundance gradient and the strength of the bar (Martin & Roy 1994; Friedli et al. 1994; Martinet & Friedli 1997). This is interpreted as the result of two effects caused by the bar: a stronger radial gas flow and hence a stronger radial mixing of metals and the efficiency of star formation. The radial mass transfer concentrates gas near the galactic center and at the ends of the bar at corotation. Enhanced star formation is the consequence of gas accumulation. The rotating bar potential also heats up the outer disk parts which leads to larger stellar velocity dispersions and a radial diffusion of stars. (Sellwood & Wilkinson 1993). Galactic bars have also been considered to support the central
infall of gas to feed a central "monster"(e.g. Beck et al. 1999).
Several authors have claimed that active galactic nuclei (AGN) are
more likely in barred galaxies than in non-barred ones (e.g. Simkin et
al. 1980; Arsenault 1989). Hummel et al. (1990) note that the fraction
of central radio sources in barred spirals is by a factor of 5 higher
than in non-barred spirals. Other authors doubt that there is a
significantly higher number of bars in galaxies harboring an AGN (e.g.
Balick & Heckman 1982; Ho et al. 1997). It appears that the
concentration of gas on a scale of One of the most famous, closest and most widely studied barred
galaxies is NGC 4303 (M61), member of the Virgo Cluster, which is
observed at an inclination of 27o (Guhathakurta et al.
1988). Optical spectra of this galaxy indicate that it consists of a
nuclear starburst and a LINER or Seyfert 2 nucleus (Filippenko &
Sargent 1986; Kennicutt et al. 1989; Colina et al. 1997; Colina &
Arribas 1999, hereafter CA99). Indications for a high star formation
rate (SFR) in NGC 4303 are given by the numerous H
II regions (Hodge & Kennicutt 1983; Martin
& Roy 1992, hereafter MR92) and three observed supernovae (van Dyk
1992). It also shows strong radio emission distributed over the entire
disk (Condon 1983). Colina et al. (1997) and CA99 discussed the
question of a starburst-AGN connection in this barred galaxy, using
optical spectroscopy and HST UV images. The data range from a nuclear
spiral structure of massive star-forming regions with an outer radius
of 225 pc down to the unresolved core of a size
VLA observations (Cayatte et al. 1990) show that NGC 4303 is
not highly H I deficient, which can be explained
by only slight environmental influences in the outermost region of the
Virgo Cluster. The projected distance to M87 is
Probable interaction companions are the nearby galaxies
NGC 4303 A (Condon 1983) and NGC 4292 (Cayatte et al.
1990), at distances of
© European Southern Observatory (ESO) 2000 Online publication: August 17, 2000 ![]() |