We present high resolution radio continuum observations of the edge-on gala
xy NGC 4631 with the Very Large Array A, BnA & B arrays in the L-, C-, and
X-band. The observed emission is limited to the inner rigidly rotating and
star forming 4 kpc-diameter disk of NGC 4631. Due to missing large-scale em
ission of the interferometric observations we detected only 7% and 12% of t
he total flux densities at L- and C-band, respectively. The spectral index
of the detected emission between L-and C-band is 0.23 (S-nu proportional to
nu(-alpha)), implying a thermal fraction of similar to 50%. We interpret t
his high thermal fraction as caused by the missing large-scale emission. Th
e non-thermal radio emission has a more extended and diffuse distribution t
o which our observations are not sensitive.
The emission is distributed asymmetrically with respect to the major axis,
the dynamical center and the center of the stellar bulge. Gravitational int
eraction may play a role causing these asymmetries. We observe no correlati
on of our radio data with H alpha data, and argue that this is likely cause
d by massive dust extinction towards the central region at optical waveleng
ths.
Point sources are identified at resolutions of 1.45 " and 0.83 " x 0.61 " i
n the central region, and their Aux densities and spectral indices are deri
ved. Two non-thermal point source complexes show strong morphological evide
nce for being external to NGC 4631; they are likely radio galaxies in the b
ackground. Alternatively, we discuss whether one of these sources may be th
e weakly active nucleus with jet-like features. Only 2-3 other point source
s are non-thermal. They may be identified with supernova remnants; Using CA
S A as a 'standard candle', we estimate a supernova rate of 0.009 yr(-1)
We estimate the thermal fraction of the total C-band radio emission of NGC
4631 with various methods, and find a likely range f(th) similar to 8-15%.
Assuming a standard IMF, the thermal fraction can be translated to a high-m
ass (M greater than or similar to, 10 M.) star formation rate of similar to
0.45-0.85 M. yr(-1), and a supernova rate of 0.03-0.056 yr(-1). This rate
is too high by a factor of three to six compared to the supernova rate esti
mated from the nonthermal point source population. it is shown that, in con
trast to NGC 4631, the supernova and star formation rates in M 82 derived w
ith the same methods agree well. Implications of the discrepancy, including
an IMF biased toward massive stars and lower average SNR luminosities in N
GC 4631 are discussed.