Morphology and kinematics of orbital components in CALIFA galaxies across the Hubble sequence

TL;DR

This study decomposes 250 CALIFA galaxies into four orbital components using Schwarzschild models, revealing how their morphology and kinematics vary across the Hubble sequence and correlating orbital fractions with galaxy types.

Contribution

It provides a detailed orbital decomposition of galaxies and links orbital components to morphological and photometric properties, challenging the use of Sersic index to distinguish bulge types.

Findings

Hotter components are more concentrated and rounder.

Component concentration and roundness increase with galaxy mass.

Orbital fractions correlate with photometric disk and bulge fractions.

Abstract

Based on the stellar orbit distribution derived from orbit-superposition Schwarzschild models, we decompose each of 250 representative present-day galaxies into four orbital components: cold with strong rotation, warm with weak rotation, hot with dominant random motion and counter-rotating (CR). We rebuild the surface brightness ($\Sigma$) of each orbital component and we present in figures and tables a quantification of their morphologies using the Sersic index \textit{n}, concentration $C = \log{(\Sigma_{0.1R_e}/\Sigma_{R_e})}$ and intrinsic flattening $q_{\mathrm{Re}}$ and $q_{\mathrm{Rmax}}$, with $R_e$ the half-light-radius and $R_{\mathrm{max}}$ the CALIFA data coverage. We find that: (1) kinematic hotter components are generally more concentrated and rounder than colder components, and (2) all components become more concentrated and thicker/rounder in more massive galaxies; they change from disk-like in low mass late-type galaxies to bulge-like in high-mass early type galaxies. Our findings suggest that Sersic \textit{n} is not a good discriminator between rotating bulges and non-rotating bulges. The luminosity fraction of cold orbits $f_{\rm cold}$ is well correlated with the photometrically-decomposed disk fraction $f_{\rm disk}$ as $f_{\mathrm{cold}} = 0.14 + 0.23f_{\mathrm{\mathrm{disk}}}$. Similarly, the hot orbit fraction $f_{\rm hot}$ is correlated with the bulge fraction $f_{\rm bulge}$ as $f_{\mathrm{hot}} = 0.19 + 0.31f_{\mathrm{\mathrm{bulge}}}$. The warm orbits mainly contribute to disks in low-mass late-type galaxies, and to bulges in high-mass early-type galaxies. The cold, warm, and hot components generally follow the same morphology ($\epsilon = 1-q_{\rm Rmax}$) versus kinematics ($\sigma_z^2/\overline{V_{\mathrm{tot}}^2}$) relation as the thin disk, thick disk/pseudo bulge, and classical bulge identified from cosmological simulations.