Revealing the spiral arms through radial migration and the shape of the metallicity distribution function
MNRAS 463, 459–466 (2016)
doi:10.1093/mnras/stw1997
Advance Access publication 2016 August 11
Revealing the spiral arms through radial migration and the shape
of the metallicity distribution function
L. A. Martinez-Medina,‹ B. Pichardo,‹ E. Moreno and A. Peimbert
Instituto de Astronomı́a, Universidad Nacional Autónoma de México, A.P. 70–264, 04510 México, CDMX, Mexico
Accepted 2016 August 5. Received 2016 August 5; in original form 2016 April 4
Recent observations show that the Milky Way’s metallicity distribution function (MDF)
changes its shape as a function of radius. This new evidence of radial migration within
the stellar disc sets additional constraints on Galactic models. By performing controlled test
particle simulations in a very detailed, observationally motivated model of the Milky Way, we
demonstrate that, in the inner region of the disc, the MDF is shaped by the joint action of the
bar and spiral arms, while at outer radii the MDF is mainly shaped by the spiral arms. We show
that the spiral arms are able to imprint their signature in the radial migration, shaping the MDF
in the outskirts of the Galactic disc with a minimal participation of the bar. Conversely, this
work has the potential to characterize some structural and dynamical parameters of the spiral
arms based on radial migration and the shape of the MDF. Finally, the resemblance obtained
with this approximation to the MDF curves of the Galaxy as seen by APOGEE, show that a
fundamental factor influencing their shape is the Galactic potential.
Key words: Galaxy: disc – Galaxy: evolution – Galaxy: kinematics and dynamics – Galaxy:
structure.
1 I N T RO D U C T I O N
An enormous effort has been dedicated, in the last decade, to the
understanding of radial and vertical orbital stellar motions induced
by the non-axisymmetric structures in the Galaxy (Sellwood &
Binney 2002; Roškar et al. 2008; Bird, Kazantzidis & Weinberg
2012; Grand, Kawata & Cropper 2012a; Roškar et al. 2012; VeraCiro et al. 2014; Halle et al. 2015; Aumer, Binney & Schönrich 2016,
and references therein). Particular attention has been paid to stellar
migration and its effects on the chemical elements distribution in the
Galaxy (Schönrich & Binney 2009; Minchev et al. 2011; Minchev,
Chiappini & Martig 2013, 2014; Sánchez-Blázquez et al. 2014;
Hayden et al. 2015; Loebman et al. 2016).
The mechanism of radial migration, as defined by Sellwood &
Binney (2002, hereafter SB02), is understood as the redistribution of
angular momentum for stars that interact with the non-axisymmetric
structure of the galaxy around the corotation (CR) resonance while
keeping their orbital eccentricity unchanged. On the other hand,
redistribution of angular momentum at radii different from CR will
cause a dynamical heating of the stellar disc. Both mechanisms
move stars to inner or outer radii, but radial migration does not
leave a kinematic imprint on stellar orbits. It is worth noting that the
E-mail: (LAMM);
(BP)
term radial migration has been used differently by different authors1
(see for example the discussion by Vera-Ciro et al. 2014).
Without the effect of stellar migration, a perfect correlation between age and metallicity of a star could be found for a given
Galactic region, assuming the abundance of chemical elements was
known in such region. Although this seems to approximate the case
for the interstellar medium (ISM) in the Milky Way (MW) and
other galaxies (Wilson & Rood 1994; Henry & Worthey 1999), it is
known that, for example, in the solar neighbourhood, stars of a given
age show a large dispersion in metallicity (Edvardsson et al. 1993).
This effect is not readily explained by plain orbital excursions from
epicycles corresponding at their birth place (SB02).
More recently, Hayden et al. (2015) measure the metallicity distribution functions (MDFs) of the MW, from a sample of 69 919
red giants from the SDSS-III/APOGEE Data Release 12. They find
that the shape of the mid-plane MDF changes systematically with
radius, with a negatively skewed distribution at 3 < R < 7 kpc, to
a roughly Gaussian distribution at the solar annulus, to a positively
skewed shape in the outer Galaxy. Using a simple model they suggest that the reversal of MDF shape could be due to radial migration.
However, a more complex model is needed to differentiate between
the contribution of the different non-axisymmetric components of
the Galaxy.
1 The results presented in this paper do not depend on the specific definition
of radial migration.
C 2016 The Authors
Published by Oxford University Press on behalf of the Royal Astronomical Society
ABSTRACT
460
L. A. Martinez-Medina et al.
With detailed orbital studies performed in suitable observationally motivated potentials of the MW, we show here that the spiral
arms can imprint their mark on the MDF.
This paper is organized as follows. The galactic model, initial
conditions, and methodology are described in Section 2. A study on
radial migration and radial heating is presented on Section 3. The
link between the MDF and the initial radial distribution is shown
in Section 4. Finally, we present the discussion and conclusions in
Sections 5 and 6.
2 THE GALAXY MODEL, NUMERICAL
S I M U L AT I O N S A N D I N I T I A L C O N D I T I O N S
(1) The model is fully adjustable. We are able to fit the whole
axisymmetric and non-axisymmetric potential (i.e. spiral arms and
bar), in three dimensions to our best understanding of the MW (or
any other particular galaxy) from observations and models.
(2) Rather than using a simple ad hoc model for a spiral perturbation, we employ a three-dimensional (3D) mass distribution for
the spiral arms, from which we derive their gravitational potential
and force fields. Our model is considerably faster, computationally
speaking, than N-body simulations.
(3) It allows us to study in great detail individual stellar orbital
behaviour (e.g. resonant regions, vertical structure, chaotic and ordered behaviour, periodic orbits to estimate at some degree orbital
self-consistency, etc.), without the resolution problems of N-body
simulations.
We have integrated test particle orbits in this 3D Galactic potential
model. Our model is observationally motivated by the MW and
suitable to explain several characteristics of the local kinematics
due to the spiral arms and the bar (such as moving groups in the
solar neighbourhood; e.g. Antoja et al. 2009).
Although the one employed is a much better suited spiral model
to represent the MW than any N-body simulation, we do not include
any prescription of metallicity or ISM physics as in Loebman et al.
(2016). In a future work, we will perform a more specific study of
the spiral arms parameters, as well as implementing a metallicity
prescription, to seek for a better fit to the APOGEE MDFs for the
MW Galaxy, and search for some restrictions to the morphology
and physical characteristics of the spiral arms.
2.1 The full Galactic model
The Galactic m (...truncated)