
2Stroe et al.
Table 1. Positions, spectroscopic redshifts (zspec), spectrum origin instrument, SDSS magnitudes in the g, r, and i bands, and
radio fluxes (at 1.4 GHz and 4.9 GHz) for each of the five HyMoRS in our sample.
Source R.A. Decl. zspec Instrument g r i S1.4 GHz S4.9GHz
hh mm ss ◦ 0 00 mag mag mag mJy mJy
J1315+516 13 14 38.12 51 34 13.4 0.47799 SDSS 20.52 ±0.03 19.75 ±0.02 18.98 ±0.02 93 51
J1348+286 13 47 51.58 28 36 29.6 0.74058 BOSS 17.39 ±0.01 17.20 ±0.01 17.43 ±0.01 241 117
J1313+507 13 13 25.78 50 42 06.2 0.88000 GMOS 21.45 ±0.05 20.96 ±0.05 20.36 ±0.04 277 84
J1154+513 11 53 46.43 51 17 04.1 1.37250 GMOS 22.10 ±0.12 21.44 ±0.11 21.37 ±0.16 495 137
J1206+503 12 06 22.39 50 17 44.3 1.45423 BOSS 21.38 ±0.04 20.89 ±0.04 20.69 ±0.05 241 75
massive red elliptical galaxies with spectra dominated
by absorption features, no broad lines, and little-to-no
narrow emission lines (e.g.; Matthews et al. 1964;Hickox
et al. 2009;Best & Heckman 2012;Janssen et al. 2012;
Butler et al. 2018). At low jet power, both FR-Is and
FR-IIs are predominantly low-excitation radio galaxies
(LERGs) (Laing et al. 1994;Mingo et al. 2022). High-
excitation radio galaxies (HERG) appear at high jet
powers, in which FR-IIs dominate. HERGs, hosted by
bluer galaxies with lower masses, higher star formation
(SF) rates (SFR), and diskier morphologies, have strong
narrow (an order of magnitude stronger than LERGs)
and, in some cases broad, emission lines (e.g.; Baum &
Heckman 1989;Zirbel & Baum 1995;Best & Heckman
2012;Miraghaei & Best 2017;Butler et al. 2018). Fi-
nally, FR-Is tend to live in denser cluster environments
than FR-II galaxies, suggesting that the density of the
intergalactic/intracluster medium could decelerate the
jets outside of the galaxy (e.g.; Prestage & Peacock 1988;
Mingo et al. 2019).
Hybrid morphology radio sources (HyMoRS) possess
both FR-I and FR-II structures, presenting a unique
opportunity to probe the conditions which cause the
dichotomy. First identified in Gopal-Krishna & Wiita
(2000), their existence suggests that the black hole en-
gine cannot alone cause the morphological differences
between FR-I’s and FR-II’s. The number of HyMoRS
candidates has rapidly grown over the past few years,
amounting to hundreds of sources and ∼5% of the re-
solved radio AGN population in modern radio surveys
(Mingo et al. 2019;Kapi´nska et al. 2017).
In this paper, using the intrinsic properties of the
host galaxy, we investigate whether orientation can give
rise to these morphological differences. As a relativistic
jet from the black hole engine travels through the host
galaxy, it may be slowed down by intervening material
in a host galaxy or travel unimpeded and slow down on
larger scales, eventually terminating in a bright hotspot
(e.g.; Kaiser & Best 2007;Mingo et al. 2019). The dis-
tribution and type of material in the galaxy could affect
how quickly the jet slows, affecting the location of the
final emission peak (Gopal-Krishna & Wiita 1996). We
aim to unveil the cause of the dichotomy by focusing our
analysis on the best-studied five sources that Gawro´nski
et al. (2006) securely identified as HyMoRS given their
spatially-resolved radio observations (see Figure 1). L-
band (1.0−2.0 GHz) images from the Very Large Array
(VLA) show the presence of one FR-I-like and one FR-II
set of structures in each system, but, using spectral ag-
ing techniques, Harwood et al. (2020) largely attribute
the FR-I-like morphology to a favorable projection of
an FR-II jet, hotspot, and lobe. We measure detailed
galaxy properties by investigating their spectral prop-
erties with newly-obtained 1D spectroscopy from the
Gemini Multi-Object Spectrograph North (GMOS-N) in
combination with MIR color diagnostics.
In Section 2, we present our new data taken with Gem-
ini, as well as archival images and spectra, and we walk
through the data reduction methods. Section 3discusses
how we analyze the spectral and ancillary data. In Sec-
tion 4, we discuss the insights into HyMoRS host galaxy
properties and the implications for the broader forma-
tion context of powerful radio galaxies. Conclusions can
be found in Section 5.
We use the ΛCDM cosmological model of a flat uni-
verse with H0= 71 km s−1Mpc−1, Ωm= 0.27, and
Ω∆= 0.73. A Salpeter (1955) initial mass function is
used throughout.
2. SAMPLE, OBSERVATIONS AND DATA
REDUCTION
2.1. HyMoRS sample
The five sources in this study have been identified as
bona-fide HyMoRS through a uniform radio selection
by Gawro´nski et al. (2006). After selecting all sources
with 1.4 GHz fluxes >20 mJy and angular size θ > 800
in five random high galactic latitude ≈16◦×16◦ar-
eas within the VLA Faint Images of the Radio Sky at
Twenty-centimeters (FIRST) survey (White et al. 1997),
Gawro´nski et al. (2006) visually selected HyMoRS can-
didates and followed them with pointed, narrow-band
VLA observations, resulting in a secure sample of five