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Kavli Institute for Cosmology, Cambridge

 

Chronicling the reionization history at $6\lesssim z \lesssim 7$ with emergent quasar damping wings. (arXiv:2401.10328v1 [astro-ph.CO])

KICC papers - Tue, 23/01/2024 - 10:30

The spectra of high-redshift ($z\gtrsim 6$) quasars contain valuable information on the progression of the Epoch of Reionization (EoR). At redshifts $z<6$, the observed Lyman-series forest shows that the intergalactic medium (IGM) is nearly ionized, while at $z>7$ the observed quasar damping wings indicate high neutral gas fractions. However, there remains a gap in neutral gas fraction constraints at $6\lesssim z \lesssim 7$ where the Lyman series forest becomes saturated but damping wings have yet to fully emerge. In this work, we use a sample of 18 quasar spectra at redshifts $6.0<z<7.1$ to close this gap. We apply neural networks to reconstruct the quasars' continuum emission around the partially absorbed Lyman $\alpha$ line to normalize their spectra, and stack these continuum-normalized spectra in three redshift bins. To increase the robustness of our results, we compare the stacks to a grid of models from two hydrodynamical simulations, ATON and CROC, and we measure the volume-averaged neutral gas fraction, $\bar{x}_{\rm HI}$, while jointly fitting for the mean quasar lifetime, $t_{\rm Q}$, for each stacked spectrum. We chronicle the evolution of neutral gas fraction using the ATON (CROC) models as follows: $\bar{x}_{\rm HI} = 0.21_{-0.07}^{+0.17}$ ($\bar{x}_{\rm HI} = 0.10_{<10^{-4}}^{+0.73}$) at $\langle z \rangle =6.10$, $\bar{x}_{\rm HI} = 0.21_{-0.07}^{+0.33}$ ($\bar{x}_{\rm HI} =0.57_{-0.47}^{+0.26}$) at $\langle z \rangle =6.46$, and $\bar{x}_{\rm HI} = 0.37_{-0.17}^{+0.17}$ ($\bar{x}_{\rm HI} =0.57_{-0.21}^{+0.26}$) at $\langle z \rangle =6.87$. At the same time we constrain the average quasar lifetime to be $t_{\rm Q} \lesssim 7\ {\rm Myr}$ across all redshift bins, in good agreement with previous studies.

Wed 24 Jan 13:15: Gravitational Instability in Irradiated Protoplanetary Discs

Upcoming Talks - Mon, 22/01/2024 - 11:13
Gravitational Instability in Irradiated Protoplanetary Discs

Young protoplanetary discs are expected to be massive and self-gravitating. The resulting gravitational instability (GI) causes large spiral structures in the disc and is a potential formation mechanism of giant planets via direct collapse of overdense regions of gas. The onset of GI is sensitive to thermal processes in the disc. It is, therefore, influenced by irradiation, such as that from the central star, which is expected to suppress the instability. However, this is dependent on the exact implementation of heating. In this talk I will present the results of 2D hydrodynamic simulations comparing the outcomes of two different heating prescriptions and show that a disc heated per unit area remains gravitationally unstable even under high levels of irradiation.

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Wed 24 Jan 13:15: The black hole mass-metallicity relation and insights into galaxy quenching

Upcoming Talks - Mon, 22/01/2024 - 11:12
The black hole mass-metallicity relation and insights into galaxy quenching

Understanding the quenching of star formation in galaxies remains a central question within extragalactic astrophysics. In this talk I will explore the intricate interplay between galaxy quenching, black hole mass, and ‘starvation’. Previous research has established a strong correlation between quiescence and black hole mass, while other studies have highlighted the role of ‘starvation’—the halting of gas inflows—as a driving force in quenching, based on rapid gas depletion through star formation and chemical enrichment. This investigation bridges the gap between these findings, shedding light on the underlying mechanisms. Leveraging an extensive dataset of galaxies, this study uses random forest regression and partial correlation coefficients to uncover the fundamental relationships governing stellar metallicity with respect to other galaxy characteristics. I will show that for actively star-forming galaxies, stellar metallicity exhibits a strong dependence on stellar mass. However, intriguingly, for passive galaxies, a dramatically different narrative emerges, where the primary driver of stellar metallicity is the black hole mass. This means the integrated impact of black hole feedback emerges as the crucial determinant, cutting off gas inflows and inducing a state of ‘starvation’, ultimately leading to the observed rapid rise in stellar metallicity. This, in turn, paves the way for the transition of a galaxy from star-forming to quiescent. This finding not only deepens our understanding of galaxy evolution but also offers key insights into the intricate mechanisms shaping the fate of galaxies across cosmic epochs.

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Einstein-Proca theory from the Einstein-Cartan formulation. (arXiv:2306.14953v2 [hep-th] UPDATED)

KICC papers - Fri, 19/01/2024 - 12:08

We construct a theory of gravity in which a propagating massive vector field arises from a quadratic curvature invariant. The Einstein-Cartan formulation and a partial suppression of torsion ensure the absence of ghost and strong-coupling problems, as we prove with nonlinear Lagrangian and Hamiltonian analysis. Augmenting General Relativity with a propagating torsion vector, our theory provides a purely gravitational origin of Einstein-Proca models and constrains their parameter space. As an outlook to phenomenology, we discuss the gravitational production of fermionic dark matter.

A small and vigorous black hole in the early Universe. (arXiv:2305.12492v2 [astro-ph.GA] UPDATED)

KICC papers - Fri, 19/01/2024 - 12:07

Multiple theories have been proposed to describe the formation of black hole seeds in the early Universe and to explain the emergence of very massive black holes observed in the first billion years after Big Bang. Models consider different seeding and accretion scenarios, which require the detection and characterisation of black holes in the first few hundred million years after Big Bang to be validated. Here we present an extensive analysis of the JWST-NIRSpec spectrum of GN-z11, an exceptionally luminous galaxy at z=10.6, revealing the detection of the [NeIV]2423 and CII*1335 transitions (typical of Active Galactic Nuclei, AGN), as well as semi-forbidden nebular lines tracing gas densities higher than 10^9 cm-3, typical of the Broad Line Region of AGN. These spectral features indicate that GN-z11 hosts an accreting black hole. The spectrum also reveals a deep and blueshifted CIV1549 absorption trough, tracing an outflow with velocity 800-1000 km/s, likely driven by the AGN. Assuming local virial relations, we derive a black hole mass of log(M_BH/Msun) = 6.2 +- 0.3, accreting at about 5 times the Eddington rate. These properties are consistent with both heavy seeds scenarios, or scenarios envisaging intermediate/light seeds experiencing episodic super-Eddington phases. Our finding naturally explains the high luminosity of GN-z11 and can also provide an explanation for its exceptionally high nitrogen abundance.

What is the nature of Little Red Dots and what is not, MIRI SMILES edition. (arXiv:2401.08782v1 [astro-ph.GA])

KICC papers - Fri, 19/01/2024 - 11:40

We study little red dots (LRD) detected by JADES and covered by the SMILES MIRI survey. Our sample contains 31 sources, $\sim70$% detected in the two bluest MIRI bands, 40% in redder filters. The median/quartiles redshifts are $z=6.9_{5.9}^{7.7}$ (55% spectroscopic). We analyze the rest-frame ultraviolet through near/mid-infrared spectral energy distributions of LRDs combining NIRCam and MIRI observations, using a variety of modeling techniques that include emission from stars, dust, and (un)obscured active galactic nuclei (AGN). The NIRCam$-$MIRI colors, for $\geq10$ $\mu$m, are bluer than direct pure emission from AGN tori; the spectral slope flattens in the rest-frame near-infrared, consistent with a 1.6 $\mu$m stellar bump. Both observations imply that stellar emission makes the dominant contribution at these wavelengths, expediting a stellar mass estimation: the median/quartiles are $\log \mathrm{M_\star/M_\odot}=9.4_{9.1}^{9.7}$. The number density of LRDs is $10^{-4.0\pm0.1}$ Mpc$^{-3}$, accounting for $14\pm3$% of the global population of galaxies with similar redshifts and masses. The flat ultraviolet spectral range is dominated by young stars. The rest-frame near/mid-infrared (2-4 $\mu$m) spectral slope reveals significant amounts of dust (bolometric stellar attenuation $\sim3-4$ mag) heated by strong radiation fields arising from highly embedded compact sources. Our models imply $<0.4$ kpc heating knots, containing dust-enshrouded OB stars or an AGN producing a similar radiation field, obscured by $\mathrm{A(V)}>10$ mag. We conclude that LRDs are extremely intense and compact starburst galaxies with mass-weighted ages 5-10 Myr, very efficient in producing dust, their global energy output dominated by the direct and dust-recycled emission from OB stars, with some contribution from obscured AGN in the mid-infrared.

The stellar Fundamental Metallicity Relation: the correlation between stellar mass, star-formation rate and stellar metallicity. (arXiv:2401.08769v1 [astro-ph.GA])

KICC papers - Fri, 19/01/2024 - 11:38

We present observational evidence for a stellar Fundamental Metallicity Relation (FMR), a smooth relation between stellar mass, star-formation rate (SFR) and the light-weighted stellar metallicity of galaxies (analogous to the well-established gas-phase FMR). We use the flexible, non-parametric software pPXF to reconstruct simultaneously the star-formation and chemical-enrichment history of a representative sample of galaxies from the local MaNGA survey. We find that (i) the metallicity of individual galaxies increases with cosmic time and (ii) at all stellar masses, the metallicity of galaxies is progressively higher, moving from the star-burst region above the main sequence (MS) towards the passive galaxies below the MS, manifesting the stellar FMR. These findings are in qualitative agreement with theoretical expectations from IllustrisTNG, where we find a mass-weighted stellar FMR. The scatter is reduced when replacing the stellar mass $M_{*}$ with $M_{*}/R_{\rm e}$ (with $R_{\rm e}$ being the effective radius), in agreement with previous results using the velocity dispersion $\sigma_{\rm e}$, which correlates with $M_{*}/R_{\rm e}$. Our results point to starvation as the main physical process through which galaxies quench, showing that metal-poor gas accretion from the intergalactic/circumgalactic medium -- or the lack thereof -- plays an important role in galaxy evolution by simultaneously shaping both their star-formation and their metallicity evolutions, while outflows play a subordinate role. This interpretation is further supported by the additional finding of a young stellar FMR, tracing only the stellar populations formed in the last 300 Myr. This suggests a tight co-evolution of the chemical composition of both the gaseous interstellar medium and the stellar populations, where the gas-phase FMR is continuously imprinted onto the stars over cosmic times.

Scalable hierarchical BayeSN inference: Investigating dependence of SN Ia host galaxy dust properties on stellar mass and redshift. (arXiv:2401.08755v1 [astro-ph.CO])

KICC papers - Fri, 19/01/2024 - 11:34

We apply the hierarchical probabilistic SED model BayeSN to analyse a sample of 475 SNe Ia (0.015 < z < 0.4) from Foundation, DES3YR and PS1MD to investigate the properties of dust in their host galaxies. We jointly infer the dust law $R_V$ population distributions at the SED level in high- and low-mass galaxies simultaneously with dust-independent, intrinsic differences. We find an intrinsic mass step of $-0.049\pm0.016$ mag, at a significance of 3.1$\sigma$, when allowing for a constant intrinsic, achromatic magnitude offset. We additionally apply a model allowing for time- and wavelength-dependent intrinsic differences between SNe Ia in different mass bins, finding $\sim$2$\sigma$ differences in magnitude and colour around peak and 4.5$\sigma$ differences at later times. These intrinsic differences are inferred simultaneously with a difference in population mean $R_V$ of $\sim$2$\sigma$ significance, demonstrating that both intrinsic and extrinsic differences may play a role in causing the host galaxy mass step. We also consider a model which allows the mean of the $R_V$ distribution to linearly evolve with redshift but find no evidence for any evolution - we infer the gradient of this relation $\eta_R = -0.38\pm0.70$. In addition, we discuss in brief a new, GPU-accelerated Python implementation of BayeSN suitable for application to large surveys which is publicly available and can be used for future cosmological analyses; this code can be found here: https://github.com/bayesn/bayesn.

Galaxy mergers solve early Universe mystery

Cosmology Papers - Fri, 19/01/2024 - 11:22

This has solved one of the most puzzling mysteries in astronomy – why astronomers detect light from hydrogen atoms that should have been entirely blocked by the pristine gas that formed after the Big Bang.

These new observations have found small, faint objects surrounding the galaxies that show the ‘inexplicable’ hydrogen emission. In conjunction with state-of-the-art simulations of galaxies in the early Universe, the observations have shown that the chaotic merging of these neighbouring galaxies is the source of this hydrogen emission. The results are reported in the journal Nature Astronomy.

Light travels at a finite speed (300 000 km a second), which means that the further away a galaxy is, the longer it has taken the light from it to reach our Solar System. As a result, not only do observations of the most distant galaxies probe the far reaches of the Universe, but they also allow us to study the Universe as it was in the past.

To study the early Universe, astronomers require exceptionally powerful telescopes that are capable of observing very distant – and therefore very faint – galaxies. One of Webb’s key capabilities is its ability to observe these galaxies, and probe the early history of the Universe.

The earliest galaxies were sites of vigorous and active star formation, and were rich sources of a type of light emitted by hydrogen atoms called Lyman-α emission. However, during the epoch of reionisation, an immense amount of neutral hydrogen gas surrounded these stellar nurseries. Furthermore, the space between galaxies was filled by more of this neutral gas than is the case today. The gas can effectively absorb and scatter this kind of hydrogen emission, so astronomers have long predicted that the abundant Lyman-α emission released in the early Universe should not be observable today.

This theory has not always stood up to scrutiny, however, as examples of early hydrogen emission have previously been observed by astronomers. This has presented a mystery: how is it that this hydrogen emission – which should have long since been absorbed or scattered – is being observed?

“One of the most puzzling issues that previous observations presented was the detection of light from hydrogen atoms in the very early Universe, which should have been entirely blocked by the pristine neutral gas that was formed after the Big Bang,” said lead author Callum Witten from Cambridge’s Institute of Astronomy. “Many hypotheses have previously been suggested to explain the great escape of this ‘inexplicable’ emission.”

The team’s breakthrough came thanks to Webb’s combination of angular resolution and sensitivity. The observations with Webb’s NIRCam instrument were able to resolve smaller, fainter galaxies that surround the bright galaxies from which the ‘inexplicable’ hydrogen emission had been detected. In other words, the surroundings of these galaxies appear to be a much busier place than we previously thought, filled with small, faint galaxies.

These smaller galaxies were interacting and merging with one another, and Webb has revealed that galaxy mergers play an important role in explaining the mystery emission from the earliest galaxies.

“Where Hubble was seeing only a large galaxy, Webb sees a cluster of smaller interacting galaxies, and this revelation has had a huge impact on our understanding of the unexpected hydrogen emission from some of the first galaxies,” said co-author Sergio Martin-Alvarez from Stanford University.

The team then used computer simulations to explore the physical processes that might explain their results. They found that the rapid build-up of stellar mass through galaxy mergers both drove strong hydrogen emission and facilitated the escape of that radiation via channels cleared of the abundant neutral gas. So, the high merger rate of the previously unobserved smaller galaxies presented a compelling solution to the long-standing puzzle of the ‘inexplicable’ early hydrogen emission.

The team is planning follow-up observations with galaxies at various stages of merging, to continue to develop their understanding of how the hydrogen emission is ejected from these changing systems. Ultimately, this will enable them to improve our understanding of galaxy evolution.

Reference:
Callum Witten et al. ‘Deciphering Lyman-α emission deep into the epoch of reionization.’ Nature Astronomy (2024). DOI: 10.1038/s41550-023-02179-3

Adapted from an ESA press release.

A team of astronomers, led by the University of Cambridge, has used the NASA/ESA/CSA James Webb Space Telescope to reveal, for the first time, what lies in the local environment of galaxies in the very early Universe.

ESA/Webb, NASA & CSA, S. Finkelstein (UT Austin), M. Bagley (UT Austin), R. Larson (UT Austin), A. Pagan (STScI), C. Witten, M. Zooming in on three neighbouring galaxies (NIRCam image)


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Wed 24 Jan 14:00: On-shell techniques for the standard-model EFTs

Upcoming Talks - Fri, 19/01/2024 - 10:07
On-shell techniques for the standard-model EFTs

Bypassing fields, operators and Lagrangians to target directly physical amplitudes advantageously avoids gauge and field-redefinition redundancies. Unitarity and analyticity allow for the construction of on-shell amplitudes, recursively in leg and loop numbers. After decades of developments focusing mostly on renormalisable theories, the associated on-shell amplitude techniques have recently been more extensively applied to effective field theories, including those which parameterise hypothetical heavy physics appearing beyond the standard model. The enumeration of independent operators can be substituted for that of contact-term amplitudes. In a given scattering, the possible kinematic structures can be fully characterised. Unitarity and analyticity allow for the derivation of positivity constraints, for the extraction of anomalous dimensions and of matching coefficients. This talk will cover some of these developments.

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Fri 02 Feb 11:30: IoA/KICC Open Day

Upcoming Talks - Thu, 18/01/2024 - 21:49
IoA/KICC Open Day

Abstract not available

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The Relation Between AGN and Host Galaxy Properties: I. Obscured AGN reside in disturbed hosts at 0<z<4. (arXiv:2401.07863v1 [astro-ph.GA])

KICC papers - Thu, 18/01/2024 - 10:35

The morphology of a galaxy is a manifestation of the complex interplay of physical processes occurring within and around it, and therefore offers indirect clues to its formation and evolution. We use both visual classification and computer vision to verify the suspected connection between galaxy merging activity - as evidenced by a close/merging galaxy pair, or tidal features surrounding an apparently singular system - and AGN activity. This study makes use of JADES JWST/NIRCam imagery, along with an unprecedentedly complete sample of AGN built using JWST/MIRI photometry in the same field. This 0.9-25 micron dataset enables constraints on the host galaxy morphologies of the broadest possible range of AGN beyond z~1, including heavily obscured examples missing from previous studies. We consider two AGN samples, one consisting of lightly to highly obscured X-ray-selected AGN (Lyu et al. 2022), and the other, presumed Compton-thick mid-infrared-bright/X-ray-faint AGN recently revealed by MIRI (Lyu et al. 2023). Both samples contain a significant fraction of host galaxies with disturbed morphologies at all redshifts sampled, and increasingly so towards higher redshift and AGN bolometric luminosity. The most obscured systems show the highest fraction of strongly disturbed host galaxies at $95\pm4$%, followed by the moderately and unobscured/lightly obscured subsets at $78\pm6$% and $63\pm6.5$%, respectively. From this pattern of disturbances, we conclude that mergers are common amongst obscured AGN, and that the obscured AGN phase may mark a period of significant SMBH growth. This finding presents tension with the leading model on AGN fueling mechanisms (Hopkins et al. 2014) that needs reconciling.

A small and vigorous black hole in the early Universe

Cosmology Papers - Thu, 18/01/2024 - 10:19

Nature, Published online: 17 January 2024; doi:10.1038/s41586-024-07052-5

A small and vigorous black hole in the early Universe

Tue 30 Jan 14:00: Transition region spectroscopy with the Hinode/EIS instrument

Upcoming Talks - Wed, 17/01/2024 - 17:08
Transition region spectroscopy with the Hinode/EIS instrument

The EUV Imaging Spectrometer observes the Sun in the 170-292 Angstrom wavelength range, which is dominated by coronal emission lines that are mainly due to iron ions. Valuable science can still be obtained from transition region ions formed in the 0.1-0.8 MK temperature range, and some recent results are presented here.

Mg VII and Si VII (formed at 0.6 MK) produce a number of lines that are widely used for diagnostics of coronal loops. However, the standard reference wavelengths for the ions’ lines are clearly discrepant with the wavelengths measured from EIS , leading to erroneous Doppler velocity measurements. I demonstrate how EIS (which does not have an absolute wavelength calibration) can be used to obtain new reference wavelengths for the lines in combination with Astrophysical infrared measurements. The new wavelengths for Mg VII and Si VII will be added to the CHIANTI database. In addition, the EIS data show that the two ions are formed at almost exactly the same temperature and the Mg/Si relative abundance is enhanced over photospheric values by about 50%.

The coolest ion observed by EIS (other than He II) is O IV , formed at 0.1 MK. It has a rich spectrum in the EIS wavelength range with more than 20 emission lines, however most of the lines are so weak they cannot be measured in normal solar conditions. A flare spectrum from 9 March 2012 is presented where the lines can be measured, and new diagnostics are presented that yield an O IV temperature of log(T/K)=5.10 and a density of log(Ne/cm^-3)=12.55 for the flare ribbon. The results are interpreted in terms of ionization and flare models.

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Mon 10 Jun 13:00: Title to be confirmed

Upcoming Talks - Wed, 17/01/2024 - 10:59
Title to be confirmed

Abstract not available

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Mon 12 Feb 13:00: How much (robust) cosmological information can we obtain from galaxy clustering?

Upcoming Talks - Tue, 16/01/2024 - 18:52
How much (robust) cosmological information can we obtain from galaxy clustering?

All large-scale structure cosmologists are faced with the question: how do we robustly extract cosmological information, such as on dark energy, gravity, and inflation, from observed tracers such as galaxies whose astrophysics is extremely complex and incompletely understood? I will describe why guaranteeing this robustness is so difficult, and how a perturbative effective-field-theory (EFT) approach offers such a guarantee when focusing on galaxy clustering on large scales. The natural next question then is: how much cosmological information is left on these large scales if we marginalize over all the free parameters introduced in the EFT ? To answer this question, I will introduce our implementation of the EFT on a lattice as an explicit field-level forward model, which can be used both for full Bayesian inference at the field level and for likelihood-free (simulation-based) inference using summary statistics. Finally, I will show first results comparing full field-level inference and summary statistics on fully nonlinear mock tracers.

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Tue 12 Mar 13:00: TBC

Upcoming Talks - Mon, 15/01/2024 - 14:03
TBC

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Tue 05 Mar 13:00: TBC

Upcoming Talks - Mon, 15/01/2024 - 14:02
TBC

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Tue 27 Feb 13:00: TBC

Upcoming Talks - Mon, 15/01/2024 - 14:02
TBC

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