A plausible Galactic spiral pattern and its rotation speed
Mon. Not. R. Astron. Soc. 350, L47–L51 (2004)
doi:10.1111/j.1365-2966.2004.07850.x
A plausible Galactic spiral pattern and its rotation speed
M. Martos,1 X. Hernandez,1 M. Yáñez,1 E. Moreno1 and B. Pichardo2
1 Instituto
de Astronomı́a, Universidad Nacional Autónoma de México A. P. 70–264, México 04510 D.F., Mexico
of Wisconsin, Department of Astronomy 475 N. Charter St. Madison, WI 53706, USA
2 University
Accepted 2004 March 17. Received 2004 March 12; in original form 2004 January 27
ABSTRACT
Key words: ISM: structure – Galaxy: fundamental parameters – Galaxy: kinematics and
dynamics – Galaxy: structure – galaxies: spiral.
1 INTRODUCTION
The comparison of near-infrared and optical images of external
galaxies reveals interesting differences. Striking examples are M81
and NGC 2997 [see pictures in Elmegreen (1981) and Block et al.
(1994), respectively]. It is common to observe a smooth, simple
two-armed K-band pattern but a more complex pattern in the optical
blue band, often suggesting more arms and bifurcations (segments
of arms that appear to be connected to a K-band arm but are not detectable in the infrared). A two-armed smooth structure underlying
a more complex morphology also appeared in the work of Grosbøl,
Pompei & Patsis (2002); in a K-band study of 53 nearby spirals, most
galaxies displayed a grand-design, two-armed, symmetric pattern in
their inner regions which often breaks up into tighter-wound, multiple arms further out. Non-linear effects were invoked to explain
such morphology.
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2004 RAS
In recent work, data from COBE-DIRBE have shed light into the
Milky Way spiral pattern. Drimmel (2000) and Drimmel & Spergel
(2001) have presented a comprehensive picture of what this pattern
is like, presenting emission profiles of the Galactic plane in the
K band and at 240 µm. The former data set, which suffers little
absorption and traces density variation in the old stellar population,
is dominated by a two-armed structure with a minimum pitch angle
of 15.5◦ . At 240 µm, the pattern is consistent with the standard fourarmed model, that corresponding to the distribution of the youngest
stellar populations delineated by H II regions.
The conventional picture of the spiral pattern of our Galaxy maps
at least four arms, named Norma, Crux–Scutum, Carina–Sagittarius
and Perseus (for a recent review, see Vallée 2002, who also reports
a likely pitch angle of 12◦ for this pattern). Additionally, features
such as the Orion spur at the solar neighbourhood have been revealed
(Georgelin & Georgelin 1976). Drimmel (2000) laid down, from the
comparison, the hypothesis that the four-armed structure is the gas
response to the two-armed ‘stellar’ pattern.
Assuming that indeed the K-band data is by far a better tracer
of mass than the optical data of spiral structure, in this work we
We report calculations of the stellar and gaseous response to a Milky Way mass distribution
model including a spiral pattern with a locus as traced by K-band observations, superimposed
on the axisymmetric components in the plane of the disc. The stellar study extends calculations
from previous work concerning the self-consistency of the pattern. The stellar response to the
imposed spiral mass is studied via computations of the central family of periodic and nearby
orbits as a function of the pattern rotation speed, p , among other parameters. A fine grid of
values of p was explored, ranging from 12 to 25 km s−1 kpc−1 . Dynamical self-consistency
is highly sensitive to p , with the best fit appearing at 20 km s−1 kpc−1 . We give an account of
recent independent pieces of theoretical and observational work that are dependent on the value
of p , all of which are consistent with the value found here: the recent star formation history of
the Milky Way, local inferences of cosmic ray flux variations and Galactic abundance patterns.
The gaseous response, which is also a function of p , was calculated via 2D hydrodynamic
simulations with the ZEUS code. For p = 20 km s−1 kpc−1 , the response to a two-armed pattern
is a structured pattern of four arms, with bifurcations along the arms and interarm features. The
pattern qualitatively resembles the optical arms observed in our Galaxy and other galaxies.
The complex gaseous pattern appears to be linked to resonances in stellar orbits. Among these,
the 4:1 resonance plays an important role, as it determines the extent of the stellar spiral pattern
in the self-consistency study presented here. Our findings seemingly confirm predictions by
Drimmel & Spergel (2001), based on K-band data.
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M. Martos et al.
corotation and the outer Lindblad resonance (OLR). For galaxies
with a bar perturbation, the extent of the main spiral was better fitted assuming it is limited by corotation and the OLR. Using H 0 =
75 km s−1 Mpc−1 , the pattern speed was found to be for the entire
sample of the order of 20 km s−1 kpc−1 and, remarkably, was not a
sensitive function of morphological type or total mass.
In the following section, we describe our results for the stellar
orbital response to the imposed spiral pattern, through which p is
determined.
2 O R B I TA L S E L F - C O N S I S T E N C Y
M O D E L L I N G , I N F E R R I N G Ωp
As in P1, our axisymmetric Galactic model is that of Allen & Santillán (1991), which includes a bulge and a flattened disc proposed by
Miyamoto & Nagai (1975), together with a massive spherical dark
halo. We coupled to this mass distribution a spiral pattern modelled
as a superposition of inhomogeneous oblate spheroids along a locus
that fits the K-band data of Drimmel (2000), with a pitch angle of
15.5◦ . P1 describes in detail the parameters of the spheroids, which
briefly are that the minor axis of the spheroids is perpendicular to the
Galactic plane and its length is 0.5 kpc, and that the major semi-axes
have a length of 1 kpc. Each spheroid has a similar mass distribution. Different density laws, linear and exponential, were analysed,
finding no important differences.
The total mass in the spiral is fixed such that the local ratio of
spiral to background (disc) force have a prescribed value. Seeking
sensible values for this ratio, we used the empirical result of Patsis,
Contopoulos & Grosbøl (1991), where self-consistent models for
12 normal spiral galaxies are presented, a sample including Sa, Sb
and Sc galaxies. Their fig. 15 shows a correlation between the pitch
angle of the spiral arms and the relative radial force perturbation.
The forcing, proportional to the pitch angle, is increasing from Sa
to Sc types in a linear fashion. For our pitch angle of 15.5◦ , the
required ratio for self-consistency is between 5 and 10 per cent. As
shown in P1, the ratio is a function of galactocentric distance R. The
authors consider strong spirals to be those in which the ratio is 6 per
cent or more.
We found that, in order to obtain relative force perturbations in the
5 to 10 per cent range, our model requires a (...truncated)