Illuminating the Sakura Web with Fluorescent Lyα Emission

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Illuminating the Sakura Web with Fluorescent Lyα Emission Sebastiano Cantalupo In collaboration with many people, including: Cosmic Structure Formation Group at ETH, MUSE GTO Team (ETH, CRAL, Leiden, AIP, IRAP, Gottingen) J. X. Prochaska, Sakura Slug, P. Madau (UCSC), F. Arrigoni-Battaia (ESO), Joe Hennawi (UCSB), M. Haehnelt (IoA)

Illuminating the Cosmic Web with Fluorescent Lyα Emission Sebastiano Cantalupo In collaboration with many people, including: Cosmic Structure Formation Group at ETH, MUSE GTO Team (ETH, CRAL, Leiden, AIP, IRAP, Gottingen) J. X. Prochaska, Sakura Slug, P. Madau (UCSC), F. Arrigoni-Battaia (ESO), Joe Hennawi (UCSB), M. Haehnelt (IoA)

Talk Outline Motivation & introduction Detecting the Cosmic Web: very latest MUSE results (and some KCWI) Comparison with models Open questions/summary

We are all familiar with the Cosmic Web as seen in hundreds of simulations. How about the real universe? How are galaxies linked to each other? What are the morphology and the small scale properties of the Cosmic Web? How do galaxies get their gas? What are the density and temperature of the Circum Galactic Medium? Movie credits: M. Vogelsberger Direct Imaging needed

The Cosmic Web in fluorescent Lyα emission: expectations log(sb) (cgs/arcsec 2 ) Simulated Lyα images at z~2.5 (20Å NB; no noise/psf) centred on a ~10 13 M sun halo hydro-simulation (RAMSES) + Radiative Transfer (RADAMESH, SC+12) QSO fluorescence Cantalupo+12-17 NB & MUSE 1h -18 MUSE medium MUSE deep -19-20 -21 UVB+Stars UVB fluorescence 2 4 6 8 cmpc How to detect it? KCWI MUSE FOV UVB+Stars +QSO 2 4 6 8 cmpc 1) Look around bright quasars 2) Stack for statistical detection (Gallego, SC+2018; see Sofia s poster on 10th floor) 3) Integrate for 100+ hours away from quasars

Highlights from Narrow-Band imaging survey of Quasar fields at z~2.3 Compact fluorescent emitters without stellar counterparts ( Dark galaxies ) SC+12, see also Marino, SC+18 CGM in emission around a bright galaxy qso (3 ) Giant Quasar Nebulae: the Slug 1 (500kpc) qso SC+12 Morphology and SB compatible with cold filaments +other 25 QSOs (FLASHLIGHT Keck+GMOS survey; Cantalupo+, in prep.; Arrigoni-Battaia, SC+, 2016) main results: - Giant Nebulae (>100kpc) are rare in NB surveys (<10%) at z~2.3, only a few found so far. - Morphology and kinematics compatible with CGM/ IGM but Surface Brightness is too high for expected gas densities (see later). Cantalupo+14, Nature then, finally, came MUSE

45 ~350 kpc MUSE observations of QSOs at z~3.5: 100% detection rate of giant nebulae! Targets: brightest radio-quiet QSOs at 3<z<4 (and two radio-loud, R1 & R2) Exposure times: 1h only total integration ( snapshot survey) Optimally extracted pseudo-nb images with QSO PSF-subtraction obtained with CubExactor (Cantalupo in prep.) All nebulae larger than 100 kpc with various morphologies. Borisova, Cantalupo+ 2016

A 3D view of the Muse Quasar Nebula 3 (MQN03), 350kpc in size: CubExtractor (Cantalupo, in prep.) + VisIt QSO PSF and continuum subtracted cube 2σ~1x10-18 cgs/arcsec 2 350kpc 10A ~ 600km/s Borisova, Cantalupo+, 2016

Latest results: hunting for the Cosmic Web around MQN03 data collected during 2016-2017 (1x2 mosaic, ~15h in deepest part): previous 1h-deep snapshot (single pointing) this image is not available in the talk online version 65 500kpc Sakura Nebula?

A statistical view: 2D Velocity maps of the Muse Quasar Nebulae - no clear signs of rotation (with some exceptions); - radio-quiet nebulae (1-17) are kinematically narrow. Borisova, Cantalupo+, 2016

How do they compare with other Lyα Nebulae and haloes? Circularly averaged SB profile QSO PSF average profile redshift-corrected (all scaled to z=3) SLUG MUSE QSOs SLUG MUSE QSOs MUSE LAEs MUSE LAEs All giant quasar nebulae have similar SB profiles both at z~2 and z~3 once redshift-corrected Borisova, Cantalupo+, 2016

How do they compare with expectations from cosmo-simulations? RAMSES (AMR) simulation of SC+14 including Lyα RT : simulated SB (a few haloes at 10 12.5-13 M sun ) is ~10-100 fainter than observed for both recombination and photon-pumping (scattering from QSO BLR) Same discrepancy in EAGLE (SPH) for maximal fluorescent emission: Tresoldi, SC & Pezzulli, in prep. EAGLE 11.6 observed 12.4 12.0 11.8 12.8 EAGLE ref high resolution Comparison with FIRE, ILLUSTRIS-TNG and reassessment of ILLUSTRIS (see Gronke & Bird 2017) in progress. High densities in CGM/IGM are needed and unresolved by cosmo-sims.

Constraining the densities and emission mechanism with HeII 1640: NB (Lyα) c

Extended HeII emission from the Slug Nebula 12 continuum subtracted cube + CubEx v1.6 6 4 2 150kpc 2σ~3x10-19 cgs/arcsec 2 c 10A ~ 600km/s Cantalupo+, in prep.

Why is HeII missing from the Slug tail? 1) Tail Lyα emission due to photon-pumping / scattering ruled out by MOSFIRE Hα (and preliminary MUSE CIII) detection tail Lyα spectrum Lyα/Hα~5-8 consistent with Case B Recombination Leibler, Cantalupo+, MNRAS submitted tail Hα spectrum qso b

Why is HeII missing from the Slug tail? High densities required 2) High densities and larger distances c ~0.08 HeII/Lyα 0 Expected HeII/Lyα ratio (a) single-density clump scenario log (HeII/Lyα) -0.5-1 -1.5-2 -2.5 D = 50 kpc D = 160 kpc -3 D = 350 kpc -3.5 D = 1 Mpc -1 0 1 2 3 4 log(nh/cm -3 ) tail tail <0.006! (b) turbulent/lognormal density distribution scenario HeII/Lyα 0.1 0.2 σ=2.9 0.5 D=1Mpc <n>=0.01 c tail (a) n clump ~10 2-10 4 cc! (depending on actual distance) (b) log(pdf) density PDF <n>=0.01 σ=2.9 SB(Lyα) Cantalupo+, in prep. log(n/cc)

Open Questions and (some) Future Directions What sets the frequency, size and luminosity of the giant quasar Nebulae? (quasar lifetime, opening angle, halo mass, redshift, quasar luminosity, ) What is the origin of the IGM/CGM clumps traced by the Nebulae? (thermal/gravitational instabilities, quasar radiation effects, ) How this affects galaxy and QSO formation? (fast gas accretion, violent disk instability, ) Exploring a larger parameter space: - include lower luminosity quasars; - extend the redshift range to 2<z<3 (not possible with MUSE, KCWI required) - Ηα followup to constrain emission mechanism and spatially resolve clumps. Improving our theoretical understanding of IGM clump-formation : - hydrodynamical and thermal stability analysis; - detailed comparison with observational data. Moving away from quasars: - detect average Cosmic Web filaments connecting galaxies and illuminated by the cosmic UVB (>100h-deep exposure with MUSE and/or KCWI).

KCWI (ongoing) snapshot survey of bright quasars at z~2.3 Targets: >10 of the brightest quasars at z~2.3 (including QSOs previously observ with NB imaging with no detectable nebulae) Preliminary results: ~100% detection rate under QSO PSF but lower SB than z~3 MUSE Quasar Nebulae (to be confirmed) > possible redshift evolution pseudo-nb pseudo-nb, QSO PSF subtracted Cantalupo+, in prep.

Where are the clumps coming from? Instabilities from filament accretion: - RAMSES 2D simulation (resolution ~5pc) of cold filaments flowing through hot gas and initially small (5%) pressure perturbation at the interface. subsonic case, adiabatic supersonic case, adiabatic Mb=2.1 lambda = 2 Rs MOVIE MOVIE Vossberg, Cantalupo & Pezzulli, in prep. (see also Mandelker et al. 2016)

Where are the clumps coming from? Instabilities from filament accretion: - RAMSES 2D simulation (resolution ~5pc) of cold filaments flowing through hot gas and initially small (5%) pressure perturbation at the interface. ~sonic case, adiabatic MOVIE Vossberg, Cantalupo & Pezzulli, in prep. (see also Mandelker et al. 2016)

Summary, some open questions and future steps We can finally directly detect the Cosmic Web on >500kpc scales with the help of quasar fluorescent emission and MUSE. Giant Lyα Nebulae are ubiquitous around bright QSOs at z~3.5 (MUSE) and apparently less frequent in NB surveys at z~2 (or just less luminous, from our KCWI preliminary data). Is this a real redshift evolution in the quasar and/or their CGM properties or due to different observational techniques? Observations of H-Lyα, H-Hα, HeII emission suggest that clumps with large densities (n>>10 cm -3 ) and small sizes (~pc) or log-normal/turbulent density distributions with large σ should be present on intergalactic scales around quasars. What is the origin of the clumps and their effect on galaxy formation and evolution? Next Future: - Finding new Cosmic Web filaments with deep MUSE observations and enlarge the parameter space for statistical studies ( snapshots ). - Hα followup of MUSE nebulae (with JWST) and/or KCWI nebulae (from the ground). - New theoretical/numerical simulations to resolve circumgalactic gas physics. - Moving away from quasars (new instruments/idea required!). Stay tuned!