{"id":500,"date":"2021-01-16T15:31:23","date_gmt":"2021-01-16T15:31:23","guid":{"rendered":"https:\/\/themes.muffingroup.com\/be\/lab3_el\/?p=500"},"modified":"2023-08-25T09:03:48","modified_gmt":"2023-08-25T09:03:48","slug":"news","status":"publish","type":"post","link":"https:\/\/xqr30.inaf.it\/index.php\/2021\/01\/16\/news\/","title":{"rendered":"News"},"content":{"rendered":"\t\t
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News from the collaboration<\/span><\/h2>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t
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June 17, 2023:<\/strong> The black hole masses and accretion rate computed for the extended XQR-30 sample has been published in the paper “XQR-30: Black hole masses and accretion rates of 42 z \u2273 6 quasars\u201d<\/a>\u00a0led by Chiara Mazzucchelli, accepted in Astronomy & Astrophysics. \u00a0<\/strong><\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t
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May 9, 2023:<\/strong> The paper describing the XQR-30 sample and its extension (E-XQR-30):\u00a0XQR-30: The ultimate XSHOOTER quasar sample at the reionization epoch<\/a>, has been accepted in MNRAS.\u00a0The paper is led by Valentina D\u2019Odorico, which is also the P.I. of the project, and co-authored by all the members of the collaboration. \u00a0<\/strong><\/div>\n
In this work, we describe the procedures adopted for the selection of the QSO candidates, the reduction of the X-Shooter spectra and some basic operations of data analysis (e.g. the determination of the intrinsic QSO emission spectrum). The sample of 42 spectra has a median effective resolving power of R ~ 11400 and 9800 in the visible and near-infrared regions of the spectrum (VIS and NIR arm of X-Shooter), respectively. The signal-to-noise ratio per 10 km\/s pixel ranges from ~11 to 114 at a wavelength of 1285 \u212b\u00a0in the rest frame, with a median value of ~29. The composite and the reduced spectra are released to the community through a public repository, and will enable a range of studies addressing outstanding questions regarding the first Gyr of the Universe.<\/div>\n
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Comparison of the properties of E-XQR-30 (star) with other spectroscopic surveys of quasars at z ~ 6 in terms of spectral resolution, median SNR and number of targets (color scale in the sidebar). The comparison samples were selected among those published to date being obtained with a given instrument and with available \u00a0median SNR values. In particular, the sample of XSHOOTER spectra in Becker et al. (2019) is a picture of the situation before the XQR-30 survey. We also note that XSHOOTER is the instrument that offers the broadest, simultaneous wavelength coverage with respect to Magellan\/FIRE (0.82-2.51 \u03bc m), Gemini\/GNIRS (0.85-2.5 \u03bc m) and Keck\/ESI (0.39-1.1 \u03bc m).<\/h6>\n
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March 28, 2023: <\/strong><\/strong> The paper “New quasar proximity zone size measurements at z ~ 6 using the enlarged XQR-30 sample\u201d<\/a> has been accepted for publication in MNRAS. This work is led by Sindhu Satyavolu, a PhD student at the Tata Institute of Fundamental Research, India.<\/strong><\/p>\n

The masses of the central black holes of z ~ 6 quasars have been measured to be around 10^9 solar mass. The existence of such supermassive black holes at a time when the universe was less than just a Gyr old remains an unsolved problem.<\/span><\/p>\n

A key component in understanding the growth of SMBHs is measuring the quasar lifetimes. One of the ways to measure quasar lifetimes at high redshift is measuring the size of their proximity zone, i.e. the region around the quasar where it dominates the radiation field.\u00a0<\/p>\n

In this paper, we present 22 new measurements of quasar proximity zones at redshifts between 5.8 and 6.6, using the enlarged XQR-30 sample. Our inferred proximity zone sizes are 2–7 physical Mpc, with a typical uncertainty of less than 0.5 physical Mpc, which, for the first time, also includes uncertainty in the quasar continuum. We find that the correlation of proximity zone sizes with the quasar UV magnitude, redshift, and the central supermassive black hole mass indicate a large diversity of quasar lifetimes. We also find a strong correlation between proximity zone sizes and the distance to the nearest metal absorber from the quasar.<\/p>\n

Two of our quasars have proximity zone sizes that are exceptionally small. The spectrum of one of these quasars, PSOJ158-14, with z=6.02<\/em>, displays, unusually for this redshift, damping wing absorption without any detectable metal lines, which could potentially originate from the neutral inter-galactic medium. The other quasar, PSOJ108+08, has a high-ionization absorber ~0.5 physical Mpc from the edge of the proximity zone.<\/p>\n

This work increases the number of proximity zone measurements available in the last stages of cosmic reionization to 87. This data will lead to better constraints on quasar lifetimes and obscuration fractions at high redshift, which in turn will help probe the seed mass and formation redshift of supermassive black holes.<\/p>\n

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Proximity zone sizes of quasars from our sample as a function of quasar magnitude and redshift. Also shown in grey are previous measurements at similar redshifts.<\/h6>\n

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March 18, 2023: A new XQR-30\u00a0 paper “The fraction and kinematics of broad absorption line quasars across cosmic time”<\/a> has been accepted for publication in the Astrophysical Journal. This work, led by Manuela Bischetti (Universit\u00e0 degli Studi di Trieste, IT), aims to\u00a0 investigate the cosmic evolution of the occurrence and kinematics of outflows driven by supermassive black holes (BHs), as traced by C IV broad absorption line (BAL) features in the quasar spectra.<\/b><\/strong><\/strong><\/div>\n
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This study exploits a large sample of 1935 quasars at z = 2.1\u22126.6 with high luminosity, drawn from the Sloan Digital Sky Survey and from the XQR-30 survey, chosen to minimise observational biases due to quasar selection criteria. By applying a homogeneous BAL identification analysis, based on employing composite template spectra to estimate the quasar intrinsic emission, we find a BAL quasar fraction close to 20% at z \u223c 2 \u2212 4, while it increases to almost 50% at z \u223c 6. The velocity and width of the BAL features also increase at \u00a0 \u00a0 z >= 4.5. We can safely exclude that the redshift evolution of the BAL properties is due to differences in terms of quasar luminosity and accretion rate.\u00a0<\/div>\n
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These results suggest significant BH feedback occurring in the 1 Gyr old Universe, likely affecting the growth of BHs and, possibly, of their host galaxies, as supported by models of early BH and galaxy evolution.<\/div>\n<\/div>\n
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March 8, 2023: In a new paper published in MNRAS, we present evidence for rapid evolution in the CIV content of the early Universe which may be linked to hydrogen reionization. The work is lead by Postdoc researcher Rebecca Davies, working at Swinburne University of Technology in Australia.<\/b><\/strong><\/strong><\/div>\n
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Absoprtion lines due to the triply ionized carbon, C IV, \u00a0trace gas in the circumgalactic and intergalactic medium around galaxies. The C IV content of the Universe is sensitive to both the overall carbon content, which is regulated by chemical enrichment and outflows, and the ionization state of carbon, which depends sensitively on the shape and strength of the ultraviolet background. The ultraviolet background is expected to change rapidly near the end of the epoch of reionization, and therefore C IV absorbers are an important probe of this transformative period in the Universe’s history.<\/div>\n
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We analysed a sample of 260 C IV absorbers from the E-XQR-30 metal absorber catalog and found that the C IV content of the Universe increased by a factor of 5 between z~5.8 and z~4.7; a period of only 300 million years (see Figure). This is significantly more rapid than the growth observed at z < 4. The large sample size enabled us to constrain the evolution of the C IV column density distribution function and show that its slope does not change significantly as a function of redshift.<\/div>\n
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Assuming that the carbon content of galaxy haloes evolves as the integral of the cosmic star formation rate density (with some delay due to stellar lifetimes and outflow travel times), we show that chemical evolution alone could plausibly explain the fast decline in C IV over 4.3 < z < 6.3. However, the C IV\/C II ratio decreases at the highest redshifts, so the accelerated decline in C IV at z < 5 may be more naturally explained by rapid changes in the gas ionization state driven by evolution of the UV background towards the end of hydrogen\u00a0reionization.<\/div>\n<\/div>\n<\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t
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November 28, 2022:\u00a0<\/strong><\/strong>Public release of the XQR-30 metal absorber catalog!<\/b><\/div>\n
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A catalog of 778 metal absorption systems in the E-XQR-30 spectra has been published in MNRAS. The absorbers cover a wide range of redshifts (2 < z < 6) and ionization states (including OI, CII, MgII, CIV, SiIV, and NV). The catalogue significantly expands on existing samples of z > 5 absorbers, especially for C IV and Si IV which are important probes of the ionizing photon background at high redshift. The catalog can be downloaded at this GitHub link:\u00a0https:\/\/github.com\/XQR-30\/Metal-catalogue<\/a>.<\/div>\n
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The size and diversity of the absorber sample is visualised in the animated figure below. Each frame of the animation adds data for one quasar in the sample. In the bottom panel, each row shows all of the absorption systems detected in one of the six primary ions across all of the E-XQR-30 spectra combined. For each system, the hue represents the energy required to ionize the relevant ion (according to the colour scale on the right). The top panel shows a zoom-in on the redshift range 5.77 < z < 6 and illustrates the range of different kinematics and ionization structures found within the absorber sample.<\/div>\n<\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t
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April 6, 2022: Huanqing Chen, a PhD student at the University of Chicago, is leading the work “Measuring the Density Fields around Bright Quasars at z~6 with XQR-30 Spectra\u201d, which has been just accepted for publication in the Astrophysical Journal.\u00a0<\/strong><\/div>\n
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In this paper, Huanqing and collaborators studied detailed features of Lyman-alpha absorption in the regions adjacent to z~6 quasars and used them to measure the density of the intergalactic medium (IGM). Measuring the density of IGM at z~6 is very challenging, due to the almost completely saturated absorption from neutral hydrogen in the Lyman-alpha forest. However, a bright quasar ionizes its surrounding reducing the neutral fraction of hydrogen near it, and creating a large zone where the Lyman-\u03b1 absorption is not saturated (called “quasar proximity zone”).\u00a0<\/div>\n
Applying a novel\u00a0method<\/a>\u00a0she recently developed for quasar proximity zones and tested on simulated quasar spectra, Huanqing and collaborators recovered the continuous large-scale density field at z~6 along 10 quasar lines of sight for the first time. The recovered density fields contain rich information about cosmology and the environment of the first quasars. In particular, the recovered density fields in this study show that on average, bright quasars at z~6 live in overdense environments, with a typical quasar halo mass of the order of 10^12-10^13 solar masses.\u00a0<\/div>\n<\/div>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t
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April 5, 2022: The paper \u201cChemical Abundance of z~6 Quasar Broad-Line Regions in the XQR-30 Sample\u201d has been accepted for publication in MNRAS. This work is led by PhD student, Samuel Lai, working with Dr. Fuyan Bian and Dr. Chiara Mazzucchelli of European Southern Observatory, as well as Prof. Christian Wolf and Dr. Christopher Onken at Australian National University.<\/strong>

The brightest quasars at redshift z ~ 6 reflect some of the most massive and fastest growing black holes with likely the largest host galaxies within the first billion years of the universe since the big bang. The chemical abundance (or metallicity) of these earliest galaxies provides clues regarding their rates of star formation, supernovae frequency, and the resulting chemical evolution. In the low-redshift universe, it\u2019s clear that properties of central black holes and host galaxies are closely intertwined. Though this relationship is not yet convincingly established at high redshift, studying metallicity in galactic nuclear material provides a window to probe the chemical properties of the reservoir of gas from which the black hole accretes.
Our study is made possible by the high signal and high resolution observations of the brightest z ~ 6 quasars by the XQR-30 survey. We were able to take advantage of the high quality spectra to measure the structure and properties of broad emission-lines originating from chemical elements at various stages of ionisation within the hot gas surrounding the black hole.
This research investigated emission lines originating from the quasar broad-line region (BLR) in close proximity to the black hole. For this study, we utilised relationships between metallicity and emission-line flux ratios in the rest-frame ultraviolet determined from photoionisation models. We measured average line ratios which are consistent with composites of low redshift quasar spectra from black holes with similar physical properties, but the line ratios are also strongly correlated with the blueshift of the CIV emission line, an indicator of emission from an outflowing component. If this outflowing contribution is not taken into account, it is possible to measure metallicity over 10 times the solar abundance at high redshift, which may indicate exotic chemical enrichment scenarios or enhanced supernova rates. Rather, our results found the metallicity of the BLR to be at least 2-4 times the solar abundance when the contribution of the blueshifted emission is minimised. While still super-solar, this lower metallicity is more readily reproduced in less extreme chemical evolution models in the galactic nuclear region. Overall, these results suggest that the BLRs of these quasars are already rapidly enriched to several times the solar abundance very early on in the universe. After which, there is no appreciable change in the metallicity for black holes with similar properties over vast swathes of cosmic time.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t

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March 9, 2022: XSHOOTER observations of the XQR-30 Large Programme have been completed!<\/strong><\/p>\n

The last OB (observing block) was observed in the night between 8 and 9 of March 2022. Observations of our Large Programme had started the 7th of April 2019. Due to the COVID pandemic there had been an interruption of operations at the ESO observatories from March 23 to October 21 2020. We are grateful to the ESO telescope operators and night astronomers \u00a0for the time they have dedicated to our program!<\/div>\n

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March 3, 2022: Discovery of strong black-hole outflows suppressing black-hole growth in quasars at redshifts 5.8-6.6, based on XQR-30 quasar spectra. Results have been published in Nature\u00a0(Bischetti M., Feruglio C., D\u2019Odorico V., et al.\u00a0Suppression of black-hole growth by strong outflows at redshifts 5.8-6.6<\/a>, 2022, Nature<\/i> 605, <\/b>244\u2013247 (2022). https:\/\/doi.org\/10.1038\/s41586-022-04608-1). This work is led by Postdoc researcher Manuela Bischetti, working at INAF Observatory of Trieste.<\/strong><\/p>\n

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Bright quasars, powered by accretion onto billion-solar-mass black holes, are among the most luminous astronomical sources. While we observe that in the nearby Universe black holes and galaxies grow together, we do not know when this common evolution started.\u00a0In this work, we observe black holes when the Universe was only 0.5-1 Gyr old, and we find that about half of them drive winds with extreme velocities, up to 17% of the speed of light, injecting large amounts of energy into the galaxy medium and slowing down black-hole growth by preventing gas accretion.\u00a0This is different from what is observed at later epochs, when black-hole winds are neither this frequent nor this energetic. The higher fraction and the extreme speed of black hole winds that we observe indicate that black hole feedback is strong in the young Universe, and may play an important role in shaping the early growth phases of both black holes and galaxies.\u00a0<\/div>\n
The large investment of time dedicated by the XQR-30 survey to observing z~6 bright quasars and the unique capacities of XSHOOTER in terms of efficiency, wavelength coverage and resolving power have allowed us to obtain very good quality spectra which enabled the interesting result obtained by Dr. Bischetti.\u00a0<\/div>\n
This research investigated black hole outflows as traced by broad absorption line (BAL) features in the XSHOOTER spectra of XQR-30 quasars. \u00a0We found that ~40-50% of the XQR-30 quasars shows the presence of BAL systems against a ~20% observed in SDSS quasars at redshift z~2-3. Furthermore, XQR-30 BAL features have much higher velocities with respect to lower redshift BAL systems implying an injection of energy in their host galaxies which is\u00a0\u00a0\u227320 times higher than the energy produced by quasars observed at later epochs. This will likely inhibit further gas accretion and slow down black-hole growth.\u00a0BAL systems at these early epochs are dusty and may be caught during an initial quenching phase of obscured accretion.\u00a0Quasars at the reionization epoch may thus be witnessing the onset of significant black-hole feedback and marking the transition from a black-hole dominated growth phase to the symbiotic growth of black-hole and host-galaxy, as observed in the nearby Universe.\u00a0<\/div>\n<\/div>\n
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Sketch of a BAL QSOs, showing dust clouds in the BAL outflow, in the nuclear dusty torus and in the host-galaxy<\/span><\/em><\/div>\n<\/div>\n
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September 14, 2021: The first paper based on the XQR-30 quasar spectra has been accepted for publication in the Astrophysical Journal, it is led by a young PhD student, Yongda Zhu, working in the group of Prof. George Becker at the University of California Riverside.<\/strong><\/p>\n

In this paper, Yongda exploits the \u201cdark gap statistics\u201d that is the presence of large portions of the spectrum where the flux is completely absorbed to constrain the properties of the Reionization process that occurred when the Universe was less than 1 Gyr old.<\/div>\n
Reionization is the last major phase transition in the history of our Universe, during which most neutral hydrogen atoms in the intergalactic medium (IGM) were ionized by ionizing UV photons from e.g., galaxies. Determining when and how reionization occurred is thus essential for understanding the formation and evolution of galaxies in the early Universe.

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This work is based on 55 high-quality spectra of quasars at redshifts 5.5<z<6.5, including new data from the XQR-30 program. The presence of long dark gaps (L\u226730 comoving Mpc\/h) in the Lyman-alpha forest may indicate neutral hydrogen islands, which are highly opaque to Lyman-alpha photons.<\/div>\n
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The results of the work by Zhu and collaborators are that about 90%, 60%, and 15% of quasar spectra exhibit long dark gaps at z=6.0, 5.8, and 5.6, respectively. The last long dark gaps persist down to z~5.3.<\/div>\n
The comparison between these results and the predictions from simulations shows that a fully ionized IGM by z=6 with a homogeneous UV background is disfavored and overall, suggests \u00a0that the signature of reionization in the form of islands of neutral hydrogen and\/or large-scale fluctuations in the ionizing background remain present in the IGM until at least z \u2243 5.3.<\/div>\n
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dark gaps<\/strong>\u00a0= contiguous regions of the spectrum where the flux is completely absorbed<\/div>\n
Lyman-alpha forest<\/strong>\u00a0= region of the quasar spectrum at shorter wavelengths with respect to the Lyman-alpha emission line\u00a0 at the redshift of the quasar populated by a \u201cforest\u201d of HI Lyman-alpha\u00a0 absorption lines due to intervening material along the line of sight. \u00a0<\/div>\n<\/div>\n
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News from the collaboration June 17, 2023: The black hole masses and accretion rate computed for the extended XQR-30 sample has been published in the paper [\u2026]<\/span><\/p>\n","protected":false},"author":1,"featured_media":44,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-500","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/posts\/500","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/comments?post=500"}],"version-history":[{"count":175,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/posts\/500\/revisions"}],"predecessor-version":[{"id":1631,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/posts\/500\/revisions\/1631"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/media\/44"}],"wp:attachment":[{"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/media?parent=500"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/categories?post=500"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/xqr30.inaf.it\/index.php\/wp-json\/wp\/v2\/tags?post=500"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}