---
title: 'MQN01: A Multiphasic Cosmic Web Node at z~3.25'
url: https://www.emergentmind.com/topics/cosmic-web-node-mqn01
type: topic
---

# MQN01: A Multiphasic Cosmic Web Node at z~3.25

MQN01, usually expanded as **MUSE Quasar Nebula 01**, is a high-redshift **massive node of the cosmic web** at \(z \simeq 3.25\), centered on the hyperluminous quasar **CTS G18.01**. In the current literature it is described variously as a **cosmic-web node**, a **protocluster**, and a **protocluster core**, reflecting the fact that the system is identified through several convergent tracers rather than a single formal catalog definition. Those tracers include a giant Ly\(\alpha\) nebula, a spectroscopically confirmed galaxy overdensity, a large excess of CO-emitting and dust-obscured galaxies, an extreme concentration of X-ray AGN, and extended X-ray emission from hot gas around the central quasar [2410.03822], [2401.04765], [2410.03933], [2508.20074].

## 1. Identification and large-scale environment

MQN01 was first associated with the bright quasar environment of **CTS G18.01** and a giant Ly\(\alpha\)-emitting structure. The ALMA survey paper describes the nebula as exceptionally extended, \(\sim 30''\) in size, corresponding to \(\sim 230\) physical kpc at \(z \simeq 3.25\), and explicitly notes its **filamentary morphology** [2401.04765]. The X-ray follow-up further characterizes MQN01 as a region containing **one of the brightest Ly\(\alpha\) nebulae** and, in that paper’s phrasing, **the largest galaxy overdensity discovered so far at \(z>3\)** [2508.20074].

Within the inner MUSE-defined core, MQN01 contains **21 galaxies with high-confidence spectroscopic redshifts** inside \(4\times 4\,{\rm cMpc}^2\) and \(|\Delta v|\le 1000\,{\rm km\,s^{-1}}\) from the quasar. The corresponding overdensity is reported as
\[
\frac{\rho}{\bar{\rho}} = 53 \pm 17,
\]
for galaxies with \(M_R\le -19.25\) mag [2410.03822]. On larger scales, the FORS2 Lyman-break-galaxy mapping covers \(\approx 24\times 24\,{\rm cMpc}^2\) and shows that the photometric overdensity is aligned with the inner spectroscopic structure and with the extended Ly\(\alpha\) morphology, suggesting that the dense inner region may continue for **a few tens of comoving Mpc** [2410.03822].

This environment is therefore not presented as a compact isolated clump. The recurring interpretation is that MQN01 marks a dense junction of filamentary gas and galaxy structure, with a highly overdense inner core embedded in a larger anisotropic overdensity [2410.03822].

## 2. Observational basis and membership definition

MQN01 has been studied through a deliberately multiwavelength program. The core spectroscopic map is a **VLT/MUSE** \(2\times 2\) mosaic of four \(1\times1\) arcmin\(^2\) pointings, with \(\sim 10\) hr per pointing on average and a final footprint of \(\approx 2\times2\) arcmin\(^2\), corresponding to \(4\times4\,{\rm cMpc}^2\) at \(z\approx 3.25\) [2410.03822]. A companion MUSE description for the X-ray work refers to a **40 hr mosaic of four 10 hr pointings** over roughly \(2\times2\,{\rm arcmin}^2\) [2410.03933]. These data provide the conservative spectroscopic backbone: membership requires at least two identifiable rest-UV spectral features, so that Ly\(\alpha\) fluorescence from the quasar does not by itself define a galaxy redshift [2410.03822].

The wider-field optical context comes from **VLT/FORS2** \(U\), \(B\), and \(R\) imaging over \(\approx 24\times24\,{\rm cMpc}^2\), yielding **535 LBG candidates** through a calibrated \(UBR\) selection [2410.03822]. Near-infrared constraints come from **VLT/HAWK-I** and **HST/ACS**, while **JWST/NIRCam** pre-imaging and **JWST/NIRSpec MSA** spectroscopy provide rest-frame optical morphology, stellar masses, SFRs, and nebular diagnostics for selected members [2410.03822], [2511.19608].

The sub-mm and molecular-gas census is based on **ALMA** Bands 3 and 6. The broad mosaic covers essentially the MUSE field, targeting CO(4–3), 3-mm continuum, and 1.2-mm continuum [2401.04765]. A later high-angular-resolution ALMA Band 3 pointing with \(\simeq 0.3''\) resolution focuses on the central \(\sim 150\,{\rm kpc}\) around the quasar [2507.16921].

The X-ray view is based on a **634 ks Chandra ACIS-I survey**. In the AGN census, the central MQN01 science region is tied to the MUSE mosaic and to spectroscopic or ALMA-confirmed members within \(\pm 1000\,{\rm km\,s^{-1}}\) of the quasar [2410.03933]. In the diffuse-halo analysis, the same Chandra dataset is re-aligned on the bright quasar itself to isolate extended soft X-ray emission after detailed PSF subtraction [2508.20074].

## 3. Molecular gas, dust, and obscured assembly

The ALMA survey established that MQN01 is not merely overdense in UV-selected galaxies. In the \( \sim 2'\times 2' \) field around the quasar, the survey identifies a **robust sample of eleven CO line-emitting galaxies** within \(\pm 4000\,{\rm km\,s^{-1}}\) of the quasar systemic redshift, including a closely separated quasar companion, and also **eleven** 1.2-mm continuum sources [2401.04765]. A fraction of these galaxies are explicitly stated to be **missed in previous deep rest-frame optical/UV surveys**, which is one reason the paper treats mm imaging as essential to the baryon census of the node [2401.04765].

The environmental contrast relative to blank fields is quantified through the CO luminosity function and continuum number counts. Above the survey limiting CO luminosity, the cumulative overdensities are reported as
\[
\delta_{\rm CO}^{4000}(>L'_{\rm lim})=14^{+9}_{-6},
\qquad
\delta_{\rm CO}^{1000}(>L'_{\rm lim})=18^{+14}_{-8},
\]
and the abstract summarizes the result as a galaxy overdensity of \(\delta>10\) [2401.04765]. The paper also finds evidence of a **systematic flattening at the bright end of the CO luminosity function** with respect to blank fields, implying that the excess is not only numerical but also weighted toward very luminous CO emitters [2401.04765].

The aggregate molecular-gas density is correspondingly large. Using the adopted CO(4–3) to CO(1–0) conversion framework, the authors derive
\[
\rho({\rm H_2})=3.7^{+1.0}_{-0.9}\times10^8\ M_\odot\,{\rm cMpc^{-3}}
\]
for the broader \(\Delta v<4000\,{\rm km\,s^{-1}}\) sample, and
\[
\rho({\rm H_2})=(1.0\pm0.3)\times10^9\ M_\odot\,{\rm cMpc^{-3}}
\]
for the secure \(\Delta v<1000\,{\rm km\,s^{-1}}\) sample without completeness correction [2401.04765]. The paper interprets this as roughly an order-of-magnitude enhancement over the expected cosmic molecular-gas density at similar redshift [2401.04765].

Within the apparent central core, the CO-member velocity distribution inside \(\Delta v_{\rm QSO}<1000\,{\rm km\,s^{-1}}\) is approximately Gaussian, with
\[
v_0 = -137^{+84}_{-86}\ {\rm km\,s^{-1}},
\qquad
\sigma = 208^{+45}_{-59}\ {\rm km\,s^{-1}},
\]
although the same paper cautions that any virial interpretation is uncertain and likely conservative [2401.04765].

## 4. AGN concentration and the hot phase

MQN01 is also exceptional as an AGN environment. Combining Chandra, MUSE, and ALMA data, the X-ray AGN census identifies **six X-ray AGN** within a region of \(16\,{\rm cMpc}^2\) and \(\pm 1000\,{\rm km\,s^{-1}}\) around the quasar, corresponding to an **X-ray AGN overdensity of \(\sim 1000\)** [2410.03933]. The same study reports an AGN fraction
\[
f_{\rm AGN} > 20\%,
\]
with the fraction increasing with stellar mass and reaching
\[
f_{\rm AGN}=1
\quad\text{for}\quad
\log(M_\*/M_\odot)>10.5
\]
in the observed sample [2410.03933].

The AGN study also characterizes the accretion intensity through the specific black-hole accretion rate
\[
\lambda_{\text{sBHAR}} = \frac{k_{\text{bol}} L_X}{1.3 \times 10^{38} \times 0.002 \times M_\*},
\]
with \(k_{\rm bol}=25\) [2410.03933]. The MQN01 AGN population is described as having a higher average \(\lambda_{\rm sBHAR}\) than the field and than the comparison protoclusters Spiderweb and SSA22, with evidence that \(\lambda_{\rm sBHAR}\) generally increases toward the center of the overdensity [2410.03933]. For the combined MQN01+Spiderweb sample, the radial trend yields mean Pearson and Spearman coefficients of \(-0.71\) and \(-0.76\), respectively [2410.03933].

A distinct but related result is the detection of **extended soft X-ray emission** around the central quasar. After PSF and background subtraction, the diffuse-halo paper reports \(\approx 66\pm 8\) net counts in the observed 0.5–2 keV band, at \(\sim 8\sigma\) significance, extending to at least \(\sim 30\) kpc from the QSO [2508.20074]. A joint spatial-spectral MCMC analysis favors thermal plasma in CIE with
\[
kT = 1.81^{+0.38}_{-0.37}\ {\rm keV},
\]
a steep \(\beta\)-model profile,
\[
\beta=2.04^{+1.35}_{-0.75},
\qquad
r_{\rm core}=36^{+16}_{-13}\ {\rm kpc},
\]
and a central electron density
\[
n_{e,0}=0.86^{+0.48}_{-0.19}\ {\rm cm^{-3}}
\]
[2508.20074].

Under the virialized-halo interpretation, the same analysis gives
\[
M_{\rm vir}\simeq (3\pm1)\times10^{13}\ M_\odot,
\qquad
R_{\rm vir}=190^{+19}_{-20}\ {\rm kpc},
\]
and a hot-gas mass
\[
M_{\rm hot}(<R_{\rm vir})=2.6^{+1.7}_{-0.6}\times10^{12}\ M_\odot,
\]
equivalent to \(8.3^{+9.8}_{-3.0}\%\) of \(M_{\rm vir}\), or \(56^{+65}_{-20}\%\) of the theoretical cosmological baryon budget of the halo [2508.20074]. The inferred X-ray luminosity is extremely high for this temperature, and the system is described as a clear outlier in the \(L_X\)-\(T_X\) plane [2508.20074].

The hot phase is also dynamically interesting. The cooling times are reported as
\[
t_{\rm cool}(15\,{\rm kpc})=55^{+24}_{-14}\ {\rm Myr},
\qquad
t_{\rm cool}(30\,{\rm kpc})=181^{+268}_{-83}\ {\rm Myr},
\]
while
\[
\frac{t_{\rm cool}}{t_{\rm ff}}(15\,{\rm kpc})=1.9^{+1.9}_{-0.9},
\qquad
\frac{t_{\rm cool}}{t_{\rm ff}}(30\,{\rm kpc})=3.1^{+4.6}_{-1.4},
\]
placing the inner halo in the commonly discussed precipitation regime [2508.20074]. This suggests a multiphase medium in which dense cool clumps and hot pressure support coexist.

## 5. Galaxy populations, chemical enrichment, and quenching

Despite the extreme environment, MQN01 does not appear to host a universal SFR enhancement at fixed stellar mass. The galaxy-growth study concludes that MQN01 members are forming stars at rates consistent with the **main sequence at \(z\approx 3\)**, and that SFR is regulated primarily by local properties correlated with stellar mass rather than by environment alone [2410.03822]. The environmental signature instead appears most strongly in the stellar-mass distribution: the high-mass end of the stellar mass function is significantly elevated relative to the field above
\[
\log(M_\star/M_\odot)\gtrsim 10.5
\]
[2410.03822]. Relative to the overdensity-scaled field expectation, the paper reports \(4\pm2\) and \(24\pm11\) times more sources in the two highest stellar-mass bins [2410.03822]. This is interpreted as evidence that massive galaxies in overdense regions build up their stellar mass **earlier or more efficiently** than galaxies in average environments [2410.03822].

The metallicity study sharpens that picture. Using **9 star-forming galaxies** with JWST/NIRSpec detections of \(\mathrm{H}\beta\), [OIII], \(\mathrm{H}\alpha\), and [NII], spanning \(10^{7.5}M_\odot\) to \(10^{10.5}M_\odot\), the paper finds that MQN01 galaxies have **higher** [NII]\(\lambda 6585\)/\(\mathrm{H}\alpha\) and **lower** [OIII]\(\lambda 5008\)/\(\mathrm{H}\beta\) than typical field galaxies at similar redshift, implying a metallicity enhancement of about
\[
0.25\pm0.07\ {\rm dex}
\]
with respect to the field mass-metallicity relation [2511.19608]. The same paper fits the MQN01 MZR with
\[
12+\log(\mathrm{O/H}) = k(\log M_\* - \log M_0) + Z_0,
\]
and for the full MQN01 sample reports \(k=0.28\pm0.08\), \(\log M_0=9.46\), \(Z_0=8.51\pm0.05\), corresponding to
\[
12+\log(\mathrm{O/H}) = 8.66 \pm 0.07
\quad\text{at}\quad
\log M_{\rm ref}=10
\]
[2511.19608]. When the fundamental metallicity relation is written through
\[
\mu_{0.60} = \log M_\* - 0.6\log\mathrm{SFR},
\]
the discrepancy with field galaxies becomes less significant, which the authors interpret as broadly consistent with accelerated or earlier stellar assembly rather than radically different regulator physics [2511.19608].

MQN01 also contains a striking quiescent counterexample to the otherwise gas-rich, star-forming node. The passive galaxy **MQN01 J004131.9-493704**, nicknamed the **Red Potato**, lies within the MQN01 structure at
\[
z = 3.2496 \pm 0.0006
\]
and has
\[
M_\star = 1.1^{+0.4}_{-0.4}\times10^{11}\ M_\odot,
\qquad
{\rm SFR}=4^{+6}_{-2}\ M_\odot\,{\rm yr}^{-1},
\]
placing it more than 1 dex below the star-forming main sequence [2601.20473]. ALMA gives no detectable molecular gas, with
\[
M_{\mathrm{H_2}} < 7\times10^{9}\ M_\odot
\]
for \(\alpha_{\rm CO}=4\), and a molecular-gas fraction
\[
f_{\mathrm{H_2}}<0.06
\]
[2601.20473]. Yet the galaxy is embedded in a large cool-gas reservoir traced by Ly\(\alpha\), H\(\alpha\), and [OIII], with an Ly\(\alpha\) halo diameter of \(\sim 80\) kpc at a surface-brightness limit of \(3\times10^{-18}\ {\rm erg\,s^{-1}\,cm^{-2}\,arcsec^{-2}}\) [2601.20473]. The favored interpretation is that inefficient gas accretion from the CGM, possibly maintained by a nearby AGN jet at projected distance \(48\) kpc, has kept the galaxy passive despite its gas-rich environment [2601.20473].

## 6. Central dynamics and physical interpretation

The central \(\sim 10\) kpc around the quasar contain a particularly informative galaxy pair. High-resolution ALMA imaging resolves a close companion, **MQN01-QC**, at approximately \(\sim 10\,{\rm kpc}\) projected distance and \(\sim -300\,{\rm km\,s^{-1}}\) from the quasar host [2507.16921]. The companion is a massive rotating disk with a clear south–north CO velocity gradient and best-fit kinematic parameters
\[
V_{\rm rot,max}=513^{+58}_{-64}\ {\rm km\,s^{-1}},
\qquad
\bar{\sigma}=46^{+12}_{-12}\ {\rm km\,s^{-1}},
\qquad
\frac{V_{\rm rot,max}}{\bar{\sigma}} = 11^{+4}_{-3},
\]
while an independent \textsc{GalPak}\(^{3D}\) analysis gives a consistent \(V_{\rm rot,max}/\sigma_0 = 10.0\pm0.2\) [2507.16921]. Its enclosed dynamical mass is
\[
M_{\rm dyn}^{\rm QC}(<4.1\,{\rm kpc}) = 2.5^{+0.6}_{-1.1}\times10^{11}\ M_\odot,
\]
and the paper highlights it as the first quasar companion galaxy confirmed as a **massive, dynamically cold rotating disk** at such an early epoch [2507.16921].

The quasar host itself is more compact and kinematically less settled. Its CO(4–3) emission contains a narrow systemic component plus a broad blueshifted wing with
\[
\Delta v\sim -300\ {\rm km\,s^{-1}},
\qquad
FWHM\sim 700\ {\rm km\,s^{-1}},
\]
which the paper interprets either as a molecular outflow or as interaction-induced disturbance [2507.16921]. Under the outflow interpretation, the estimated molecular outflow rate is
\[
\dot{M}_{\rm H2} \simeq 1.7\times10^{3}\,(\alpha_{\rm CO}/0.5)\ M_\odot\,{\rm yr^{-1}},
\]
with an outflow depletion time of \(\sim 20\) Myr [2507.16921].

At larger scales, the system is manifestly multiphase. Cold molecular gas, dust, UV-selected galaxies, X-ray AGN, giant Ly\(\alpha\) emission, and hot soft X-ray plasma all coexist within the same node. Different analyses, however, probe different scales and dynamical states. The ALMA core study reports a tentative virialized-core estimate of
\[
M_{200}=2.2^{+4.0}_{-1.8}\times10^{12}\ M_\odot
\]
from the central CO-member kinematics [2401.04765], whereas the diffuse X-ray halo interpretation yields
\[
M_{\rm vir}\simeq (3\pm1)\times10^{13}\ M_\odot
\]
for the hot halo around the quasar [2508.20074]. This suggests that current mass estimates for MQN01 are strongly **method- and aperture-dependent**, and that the node is better understood as a forming, structured overdensity than as a single relaxed halo.

A recurrent misconception is that MQN01 is simply a quasar field or, conversely, that it is already a mature cluster in the low-redshift sense. The published evidence supports neither simplification. The system is quasar-centered, but its defining properties are environmental: a spectroscopic galaxy overdensity, a CO and dust excess, an extreme AGN concentration, and a hot halo embedded in a filamentary Ly\(\alpha\) structure [2410.03822], [2401.04765], [2410.03933], [2508.20074]. At the same time, its internal diversity is pronounced: ordinary main-sequence star formers, chemically advanced massive galaxies, a passive massive galaxy in bright cool CGM, a dynamically cold massive disk, and a disturbed quasar host all coexist within the same node [2511.19608], [2601.20473], [2507.16921].

Taken together, MQN01 is best characterized as a **gas-rich, AGN-rich, chemically evolved, multiphase cosmic-web node at \(z\sim 3.25\)**, in which accelerated mass assembly is already evident at the high-mass end even though star formation at fixed stellar mass remains broadly consistent with the \(z\sim 3\) main sequence.

Source: https://www.emergentmind.com/topics/cosmic-web-node-mqn01