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QSO J1342+0928 , the SIMBAD biblio (115 results) | C.D.S. - SIMBAD4 rel 1.8 - 2024.04.19CEST17:05:14 |
Bibcode/DOI | Score |
in Title|Abstract| Keywords |
in a table | in teXt, Caption, ... | Nb occurence | Nb objects in ref |
Citations (from ADS) |
Title | First 3 Authors |
---|---|---|---|---|---|---|---|---|---|
2017ApJ...851L...8V | 888 | A | S X C | 20 | 9 | 107 | Copious amounts of dust and gas in a z = 7.5 quasar host galaxy. | VENEMANS B.P., WALTER F., DECARLI R., et al. | |
2018Natur.553..473B | 247 | 3 | 743 | An 800-million-solar-mass black hole in a significantly neutral Universe at a redshift of 7.5. | BANADOS E., VENEMANS B.P., MAZZUCCHELLI C., et al. | ||||
2018ApJ...854...97D | 20 | D | 1 | 50 | 209 | An ALMA [C II] survey of 27 quasars at z > 5.94. | DECARLI R., WALTER F., VENEMANS B.P., et al. | ||
2018ApJ...856L..25B | 1188 | T K A | X C | 27 | 3 | 33 |
Chandra X-rays from the redshift 7.54 quasar ULAS J1342+0928. |
BANADOS E., CONNOR T., STERN D., et al. | |
2018ApJ...857...22L | 92 | X | 1 | 1 | 51 | The dramatic size and kinematic evolution of massive early-type galaxies. | LAPI A., PANTONI L., ZANISI L., et al. | ||
2018MNRAS.477.3694B | 123 | X | 3 | 3 | 1 | Maximally rotating supermassive stars at the onset of collapse: the perturbative effects of gas pressure, magnetic fields, dark matter, and dark energy. | BUTLER S.P., LIMA A.R., BAUMGARTE T.W., et al. | ||
2018A&A...615A.113M | 1095 | T A | S X C | 24 | 5 | 1 |
J1342+0928 supports the timeline in the Rh = ct cosmology. |
MELIA F. | |
2018MNRAS.478.5564B | 68 | A | X | 2 | 2 | 4 | Imprints of quasar duty cycle on the 21-cm signal from the Epochof Reionization. | BOLGAR F., EAMES E., HOTTIER C., et al. | |
2018ApJ...864..142D | 1212 | A | D | S X C | 26 | 2 | 202 | Quantitative constraints on the reionization history from the IGM damping wing signature in two quasars at z > 7. | DAVIES F.B., HENNAWI J.F., BANADOS E., et al. |
2018ApJ...864..143D | 1264 | A | X | 31 | 10 | 52 | Predicting quasar continua near Lyα with principal component analysis. | DAVIES F.B., HENNAWI J.F., BANADOS E., et al. | |
2018ApJ...865..126S | 322 | A | X C | 7 | 3 | 27 | Radiation hydrodynamical simulations of the first quasars. | SMIDT J., WHALEN D.J., JOHNSON J.L., et al. | |
2018A&A...617A.127P | 66 | A | X | 2 | 20 | 1 | High-redshift quasar selection from the CFHQSIR survey. | PIPIEN S., CUBY J.-G., BASA S., et al. | |
2018ApJ...866..159V | 16 | D | 1 | 98 | 72 | Dust emission in an accretion-rate-limited sample of z >= 6 quasars. | VENEMANS B.P., DECARLI R., WALTER F., et al. | ||
2018ApJ...868...15T | 82 | C | 1 | 9 | 6 | Super-Eddington accretion in the WISE-selected extremely luminous infrared galaxy W2246-0526. | TSAI C.-W., EISENHARDT P.R.M., JUN H.D., et al. | ||
2018MNRAS.481.4877N | 317 | T A | X C F | 5 | 2 | 9 |
Gas outflows from the z = 7.54 quasar: predictions from the BLUETIDES simulation. |
NI Y., DI MATTEO T., FENG Y., et al. | |
2019ApJ...870L..11F | 93 | C | 1 | 8 | 73 | The discovery of a gravitationally lensed quasar at z = 6.51. | FAN X., WANG F., YANG J., et al. | ||
2019MNRAS.483.1388T | 800 | X C | 18 | 1 | 6 | A tiny host galaxy for the first giant black hole: z = 7.5 quasar in BlueTides. | TENNETI A., WILKINS S.M., DI MATTEO T., et al. | ||
2019MNRAS.483.4080R | 42 | X | 1 | 4 | 3 | Dark matter model favoured by reionization data: 7 keV sterile neutrino versus cold dark matter. | RUDAKOVSKYI A. and IAKUBOVSKYI D. | ||
2019MNRAS.484.3897K | 43 | X | 1 | 8 | 8 | Evidence for short ∼ 1 Myr lifetimes from the He II proximity zones of z ∼ 4 quasars. | KHRYKIN I.S., HENNAWI J.F. and WORSECK G. | ||
2019MNRAS.484.5094G | 1373 | T A | X C F | 29 | 2 | 104 |
Constraints on reionization from the z = 7.5 QSO ULAS J1342+0928. |
GREIG B., MESINGER A. and BANADOS E. | |
2019MNRAS.484.5142P | 60 | D | X | 2 | 7 | 12 | A new bright z = 6.82 quasar discovered with VISTA: VHS J0411-0907. | PONS E., McMAHON R.G., SIMCOE R.A., et al. | |
2019ApJ...872L..29S | 84 | C | 1 | 26 | 2 | Black versus dark: rapid growth of supermassive black holes in dark matter halos at z ∼ 6. | SHIMASAKU K. and IZUMI T. | ||
2019A&A...623A..92S | 84 | C | 1 | 126 | 60 | The X-shooter GRB afterglow legacy sample (XS-GRB). | SELSING J., MALESANI D., GOLDONI P., et al. | ||
2019ApJ...875...67M | 255 | X | 6 | 2 | 9 | Results from EDGES HigH-band. III. New constraints on parameters of the early universe. | MONSALVE R.A., FIALKOV A., BOWMAN J.D., et al. | ||
2019A&A...624L..13L | 170 | X | 4 | 14 | 54 | Dust production scenarios in galaxies at z ∼6-8.3. | LESNIEWSKA A. and MICHALOWSKI M.J. | ||
2019MNRAS.486.1763F | 204 | X | 2 | 1 | 120 | Signature of excess radio background in the 21-cm global signal and power spectrum. | FIALKOV A. and BARKANA R. | ||
2019A&A...625A..23C | 1421 | A | D | X C | 34 | 5 | 1 | Black hole mass and spin estimates of the most distant quasars. | CAMPITIELLO S., CELOTTI A., GHISELLINI G., et al. |
2019ApJ...878...12H | 43 | X | 1 | 83 | 128 | Constraining the neutral fraction of hydrogen in the IGM at redshift 7.5. | HOAG A., BRADAC M., HUANG K., et al. | ||
2019MNRAS.487.2030L | 42 | X | 1 | 2 | ~ | Cosmological test using the high-redshift detection rate of FSRQs with the Square Kilometre Array. | LEAF K. and MELIA F. | ||
2019MNRAS.487.3305M | 17 | D | 1 | 230 | 47 | New constraints on quasar evolution: broad-line velocity shifts over 1.5 <= z <= 7.5. | MEYER R.A., BOSMAN S.E.I. and ELLIS R.S. | ||
2019ApJ...879..117K | 59 | D | X | 2 | 52 | ~ | High star formation rates of low Eddington ratio quasars at z >= 6. | KIM Y. and IM M. | |
2019MNRAS.488.1035K | 68 | X | 1 | 6 | 156 | Evolution of the AGN UV luminosity function from redshift 7.5. | KULKARNI G., WORSECK G. and HENNAWI J.F. | ||
2019A&A...627A..72G | 42 | X | 1 | 12 | ~ | A NuSTAR view of powerful γ-ray loud blazars. | GHISELLINI G., PERRI M., COSTAMANTE L., et al. | ||
2019ApJ...880...77O | 173 | X C | 3 | 13 | 89 | Subaru high-z exploration of low-luminosity quasars (SHELLQs). VI. Black hole mass Measurements of six quasars at 6.1 <= z <= 6.7. | ONOUE M., KASHIKAWA N., MATSUOKA Y., et al. | ||
2019ApJ...881L..23B | 750 | T K A | X C | 16 | 2 | 28 |
The z = 7.54 quasar ULAS J1342+0928 is hosted by a galaxy merger. |
BANADOS E., NOVAK M., NEELEMAN M., et al. | |
2019ApJ...881...63N | 1842 | T K A | X C | 42 | 3 | 61 |
An ALMA multiline survey of the interstellar medium of the redshift 7.5 quasar host galaxy J1342+0928. |
NOVAK M., BANADOS E., DECARLI R., et al. | |
2019A&A...628L...6V | 42 | X | 1 | 5 | ~ | Discovery of the first heavily obscured QSO candidate at z > 6 in a close galaxy pair. | VITO F., BRANDT W.N., BAUER F.E., et al. | ||
2019MNRAS.488.4004L | 70 | X | 1 | 2 | 57 | High-redshift quasars and their host galaxies - I. Kinematical and dynamical properties and their tracers. | LUPI A., VOLONTERI M., DECARLI R., et al. | ||
2019MNRAS.488.4195D | 84 | X | 2 | 4 | ~ | Maximally rotating supermassive stars at the onset of collapse: effects of gas pressure. | DENNISON K.A., BAUMGARTE T.W. and SHAPIRO S.L. | ||
2019ApJ...882...77C | 17 | D | 3 | 73 | 40 | Heavy element absorption systems at 5.0 < z < 6.8: metal-poor neutral gas and a diminishing signature of highly ionized circumgalactic matter. | COOPER T.J., SIMCOE R.A., COOKSEY K.L., et al. | ||
2019A&A...630A.118V | 61 | D | X | 2 | 28 | 69 | The X-ray properties of z > 6 quasars: no evident evolution of accretion physics in the first Gyr of the Universe. | VITO F., BRANDT W.N., BAUER F.E., et al. | |
2019ApJ...884L..19D | 887 | A | X C | 20 | 2 | 53 | Evidence for low radiative efficiency or highly obscured growth of z > 7 quasars. | DAVIES F.B., HENNAWI J.F. and EILERS A.-C. | |
2019A&A...631A..85E | 102 | X | 2 | 2 | 37 | Euclid preparation. V. Predicted yield of redshift 7 < z < 9 quasars from the wide survey. | EUCLID COLLABORATION, BARNETT R., WARREN S.J., et al. | ||
2019A&A...631A.167D | 87 | C | 1 | 10 | 32 | A dense, solar metallicity ISM in the z = 4.2 dusty star-forming galaxy SPT 0418-47. | DE BREUCK C., WEISS A., BETHERMIN M., et al. | ||
2019MNRAS.489.5225I | 84 | X | 2 | 2 | ~ | AGN radiative feedback in the early growth of massive black holes. | ISHIBASHI W. | ||
2019ApJ...886...92L | 42 | X | 1 | 1 | ~ | Growth of massive black holes at high-z via accretion predominantly driven by magnetic outflows. | LI J. and CAO X. | ||
2019MNRAS.490.2542P | 17 | D | 1 | 2245 | ~ | Unveiling the weak radio quasar population at z≥4. | PERGER K., FREY S., GABANYI K.E., et al. | ||
2019A&A...632A.109N | 42 | X | 1 | 33 | 29 | The most luminous blue quasars at 3.0 < z < 3.3. I. A tale of two X-ray populations. | NARDINI E., LUSSO E., RISALITI G., et al. | ||
2019MNRAS.490.4502V | 209 | X C | 4 | 11 | ~ | Impact of X-rays on CO emission from high-z galaxies. | VALLINI L., TIELENS A.G.G.M., PALLOTTINI A., et al. | ||
2019ApJ...887..174V | 125 | X C | 2 | 3 | ~ | Submillimeter signatures from growing supermassive black holes before reionization. | VASILIEV E.O. and SHCHEKINOV Y.A. | ||
2020MNRAS.491.3884P | 238 | A | X | 6 | 14 | ~ | X-ray properties of z >= 6.5 quasars. | PONS E., McMAHON R.G., BANERJI M., et al. | |
2020MNRAS.493.3732D | 64 | X | 1 | 2 | 42 | Star formation in accretion discs and SMBH growth. | DITTMANN A.J. and MILLER M.C. | ||
2020MNRAS.493.4256D | 2324 | A | X C | 54 | 7 | ~ | Reionization history constraints from neural network based predictions of high-redshift quasar continua. | DUROVCIKOVA D., KATZ H., BOSMAN S.E.I., et al. | |
2020ApJ...892..109N | 134 | X | 1 | 2 | 183 | Rapid reionization by the oligarchs: the case for massive, uv-bright, star-forming galaxies with high escape fractions. | NAIDU R.P., TACCHELLA S., MASON C.A., et al. | ||
2020ApJS..247...69E | 47 | X | 1 | 17 | 68 | The CatWISE Preliminary Catalog: motions from WISE and NEOWISE data. | EISENHARDT P.R.M., MAROCCO F., FOWLER J.W., et al. | ||
2020MNRAS.494..789R | 60 | D | X | 2 | 489 | 25 | The near and mid-infrared photometric properties of known redshift z >= 5 quasars. | ROSS N.P. and CROSS N.J.G. | |
2020ApJ...895...74N | 17 | D | 1 | 41 | 15 | ALMA observations of quasar host galaxies at z ≃ 4.8. | NGUYEN N.H., LIRA P., TRAKHTENBROT B., et al. | ||
2020ApJ...895..130B | 85 | X | 2 | 16 | ~ | Cosmic spin and mass evolution of black holes and its impact. | BHATTACHARYYA D. and MANGALAM A. | ||
2020ApJ...896...23W | 271 | X C | 5 | 6 | 97 | A significantly neutral intergalactic medium around the luminous z = 7 quasar J0252-0503. | WANG F., DAVIES F.B., YANG J., et al. | ||
2020MNRAS.495.4845C | 84 | X | 1 | 1 | 41 | Emulating the global 21-cm signal from Cosmic Dawn and Reionization. | COHEN A., FIALKOV A., BARKANA R., et al. | ||
2020ApJ...896..151R | 85 | X | 2 | 44 | 12 | Survey of extremely high-velocity outflows in Sloan Digital Sky Survey quasars. | RODRIGUEZ HIDALGO P., KHATRI A.M., HALL P.B., et al. | ||
2020MNRAS.496..888N | 102 | D | X | 3 | 8 | ~ | Effects of the Hubble parameter on the cosmic growth of the first quasars. | NUNES R.C. and PACUCCI F. | |
2020ApJ...897L..14Y | 321 | A | X C | 6 | 5 | 200 | Poniua'ena: a luminous z > 7.5 quasar hosting a 1.5 billion solar mass black hole. | YANG J., WANG F., FAN X., et al. | |
2020MNRAS.496.1115B | 43 | X | 1 | 4 | ~ | Accretion disc luminosity for black holes surrounded by dark matter. | BOSHKAYEV K., IDRISSOV A., LUONGO O., et al. | ||
2020ApJ...898..105O | 2896 | T A | X C | 66 | 2 | 36 |
No redshift evolution in the broad-line-region metallicity up to z = 7.54: deep near-infrared spectroscopy of ULAS J1342+0928. |
ONOUE M., BANADOS E., MAZZUCCHELLI C., et al. | |
2020ApJ...900..131L | 767 | X C | 17 | 10 | 19 | Ionized and atomic interstellar medium in the z = 6.003 quasar SDSS J2310+1855. | LI J., WANG R., COX P., et al. | ||
2020MNRAS.498.6083E | 56 | X | 1 | 2 | 27 | Large-scale simulations of H and He reionization and heating driven by stars and more energetic sources. | EIDE M.B., CIARDI B., GRAZIANI L., et al. | ||
2020A&A...642A.150L | 102 | D | X | 3 | 2429 | 92 | Quasars as standard candles. III. Validation of a new sample for cosmological studies. | LUSSO E., RISALITI G., NARDINI E., et al. | |
2020ApJ...903L..18Z | 17 | D | 1 | 14 | ~ | Effects of spin on constraining the seeds and growth of >=109M☉ supermassive black holes in z > 6.5 quasars. | ZHANG X., LU Y. and FANG T. | ||
2020ApJ...904..111K | 43 | X | 1 | 45 | 26 | The Infrared Medium-deep Survey. VIII. Quasar luminosity function at z ∼ 5. | KIM Y., IM M., JEON Y., et al. | ||
2020ApJ...904..130V | 231 | D | S X | 5 | 54 | 75 | Kiloparsec-scale ALMA imaging of [C II] and dust continuum emission of 27 quasar host galaxies at z ∼ 6. | VENEMANS B.P., WALTER F., NEELEMAN M., et al. | |
2020ApJ...904..131N | 61 | D | X | 2 | 28 | 36 | No evidence for [C II] halos or high-velocity outflows in z >= 6 quasar host galaxies. | NOVAK M., VENEMANS B.P., WALTER F., et al. | |
2020ApJ...905...51S | 699 | D | S X C | 15 | 42 | 62 | The X-SHOOTER/ALMA sample of quasars in the epoch of reionization. I. NIR spectral modeling, iron enrichment, and broad emission line properties. | SCHINDLER J.-T., FARINA E.P., BANADOS E., et al. | |
2021ApJ...907L...1W | 119 | C | 1 | 7 | 230 | A luminous quasar at redshift 7.642. | WANG F., YANG J., FAN X., et al. | ||
2021ApJ...908...53W | 324 | D | X | 8 | 13 | 37 | Revealing the accretion physics of supermassive black holes at redshift z ∼ 7 with Chandra and infrared observations. | WANG F., FAN X., YANG J., et al. | |
2021MNRAS.501.4289Z | 148 | D | X F | 3 | 12 | ~ | High-redshift SMBHs can grow from stellar-mass seeds via chaotic accretion. | ZUBOVAS K. and KING A. | |
2021ApJ...908..235I | 45 | X | 1 | 7 | 11 | Subaru high-z exploration of low-luminosity quasars (SHELLQs). XII. Extended [C II] structure (merger or outflow) in a z = 6.72 Red quasar. | IZUMI T., ONOUE M., MATSUOKA Y., et al. | ||
2021ApJ...911..141N | 281 | D | X | 7 | 28 | 58 | The kinematics of z >= 6 quasar host galaxies. | NEELEMAN M., NOVAK M., VENEMANS B.P., et al. | |
2021ApJ...914...36I | 281 | D | X | 7 | 15 | 33 | Subaru high-z exploration of low-luminosity quasars (SHELLQs). XIII. Large-scale feedback and star formation in a low-luminosity quasar at z = 7.07 on the local black hole to host mass relation. | IZUMI T., MATSUOKA Y., FUJIMOTO S., et al. | |
2021ApJ...914L..26F | 20 | D | 1 | 10 | 33 | Seeding supermassive black holes with self-interacting dark matter: a unified scenario with baryons. | FENG W.-X., YU H.-B. and ZHONG Y.-M. | ||
2021MNRAS.506..613S | 50 | X | 1 | 5 | 33 | Light, medium-weight, or heavy? The nature of the first supermassive black hole seeds. | SASSANO F., SCHNEIDER R., VALIANTE R., et al. | ||
2021A&A...652A..23F | 17 | D | 1 | 66 | 8 | Measuring chemical abundances with infrared nebular lines: HII-CHI-MISTRY-IR. | FERNANDEZ-ONTIVEROS J.A., PEREZ-MONTERO E., VILCHEZ J.M., et al. | ||
2021A&A...652A..66P | 306 | X C | 6 | 21 | 27 | ALMA multiline survey of the ISM in two quasar host-companion galaxy pairs at z > 6. | PENSABENE A., DECARLI R., BANADOS E., et al. | ||
2021MNRAS.508.1262M | 44 | X | 1 | 2 | ~ | Extracting the astrophysics of reionization from the Lyα forest power spectrum: a first forecast. | MONTERO-CAMACHO P. and MAO Y. | ||
2021ApJ...919..120M | 49 | X | 1 | 7 | 37 | The evolution of the Lyman-alpha luminosity function during reionization. | MORALES A.M., MASON C.A., BRUTON S., et al. | ||
2021MNRAS.508.1973M | 54 | X | 1 | 4 | 40 | Seeds don't sink: even massive black hole 'seeds' cannot migrate to galaxy centres efficiently. | MA L., HOPKINS P.F., MA X., et al. | ||
2021A&A...656A.137G | 17 | D | 1 | 493 | 12 | Low frequency radio properties of the z > 5 quasar population. | GLOUDEMANS A.J., DUNCAN K.J., ROTTGERING H.J.A., et al. | ||
2022MNRAS.509.1885P | 92 | F | 1 | 7 | 15 | The search for the farthest quasar: consequences for black hole growth and seed models. | PACUCCI F. and LOEB A. | ||
2021ApJ...923..229G | 63 | X | 1 | 1 | 19 | SILVERRUSH. XI. Constraints on the Lyα luminosity function and cosmic reionization at z = 7.3 with Subaru/Hyper Suprime-Cam. | GOTO H., SHIMASAKU K., YAMANAKA S., et al. | ||
2022MNRAS.511..616T | 50 | X | 1 | 5 | 27 | The low-end of the black hole mass function at cosmic dawn. | TRINCA A., SCHNEIDER R., VALIANTE R., et al. | ||
2022ApJ...926..114O | 45 | X | 1 | 24 | 8 | Conditions for Direct Black Hole Seed Collapse near a Radio-loud Quasar 1 Gyr after the Big Bang. | OVERZIER R.A. | ||
2022MNRAS.512.5390G | 1063 | A | S X C F | 21 | 4 | 24 | IGM damping wing constraints on reionization from covariance reconstruction of two z >= 7 QSOs. | GREIG B., MESINGER A., DAVIES F.B., et al. | |
2022ApJ...927..152M | 47 | X | 1 | 8 | 22 | Physical Constraints on the Extended Interstellar Medium of the z = 6.42 Quasar J1148+5251: [C II]158µm, [N II]205µm, and [O I]146µm Observations. | MEYER R.A., WALTER F., CICONE C., et al. | ||
2022ApJ...927..237I | 49 | X | 1 | 4 | 19 | Rapid Growth of Seed Black Holes during Early Bulge Formation. | INAYOSHI K., NAKATANI R., TOYOUCHI D., et al. | ||
2022ApJ...928..179L | 358 | X C | 7 | 25 | 2 | Multiphase ISM in the z = 5.7 Hyperluminous Starburst SPT 0346-52. | LITKE K.C., MARRONE D.P., ARAVENA M., et al. | ||
2022Natur.604..261F | 2 | 12 | 32 | A dusty compact object bridging galaxies and quasars at cosmic dawn. | FUJIMOTO S., BRAMMER G.B., WATSON D., et al. | ||||
2022MNRAS.513.1801L | 63 | D | X | 2 | 27 | 14 | Chemical abundance of z ∼ 6 quasar broad-line regions in the XQR-30 sample. | LAI S., BIAN F., ONKEN C.A., et al. | |
2022ApJ...929..161W | 46 | X | 1 | 4 | 7 | ALMA Detections of [O III] and [C II] Emission Lines From A1689-zD1 at z = 7.13. | WONG Y.H.V., WANG P., HASHIMOTO T., et al. | ||
2022MNRAS.514.5583Z | 225 | X C | 4 | 5 | 8 | The formation of the first quasars: the black hole seeds, accretion, and feedback models. | ZHU Q., LI Y., LI Y., et al. | ||
2022A&A...662A..60D | 45 | X | 1 | 40 | 17 | Molecular gas in z ∼ 6 quasar host galaxies. | DECARLI R., PENSABENE A., VENEMANS B., et al. | ||
2022MNRAS.515.3224N | 242 | D | X F | 5 | 16 | 3 | Paving the way forEuclid and JWST via probabilistic selection of high-redshift quasars. | NANNI R., HENNAWI J.F., WANG F., et al. | |
2022ApJ...937...19Z | 45 | X | 1 | 30 | 2 | Radio Jet Proper-motion Analysis of Nine Distant Quasars above Redshift 3.5. | ZHANG Y., AN T., FREY S., et al. | ||
2022ApJ...937...61Y | 2644 | A | D | S X C | 58 | 4 | 6 | Potential Signature of Population III Pair-instability Supernova Ejecta in the BLR Gas of the Most Distant Quasar at z = 7.54. | YOSHII Y., SAMESHIMA H., TSUJIMOTO T., et al. |
2022ApJ...941..106F | 242 | D | X | 6 | 41 | 26 | The X-shooter/ALMA Sample of Quasars in the Epoch of Reionization. II. Black Hole Masses, Eddington Ratios, and the Formation of the First Quasars. | FARINA E.P., SCHINDLER J.-T., WALTER F., et al. | |
2022PASP..134l1001M | 228 | X | 5 | 1 | 4 | A Candid Assessment of Standard Cosmology. | MELIA F. | ||
2023ApJ...946L..45T | 48 | X | 1 | 3 | 5 | Accurate Dust Temperature and Star Formation Rate in the Most Luminous z > 6 Quasar in the Hyperluminous Quasars at the Epoch of Reionization (HYPERION) Sample. | TRIPODI R., FERUGLIO C., KEMPER F., et al. | ||
2023MNRAS.521.2526K | X * | 1 | 6 | 4 | A solar metallicity galaxy at z > 7? Possible detection of the [N II] 122 μm and [O III] 52 μm lines. | KILLI M., WATSON D., FUJIMOTO S., et al. | |||
2023MNRAS.519.3027S | 47 | X | 1 | 4 | 1 | Probing quasar lifetimes with proximate 21-centimetre absorption in the diffuse intergalactic medium at redshifts z ≥ 6. | SOLTINSKY T., BOLTON J.S., MOLARO M., et al. | ||
2023MNRAS.520..740F | 47 | X | 1 | 4 | 3 | Eddington accreting black holes in the epoch of reionization. | FONTANOT F., CRISTIANI S., GRAZIAN A., et al. | ||
2023MNRAS.523.3119W | 19 | D | 2 | 27 | 1 | An empirical study of dust properties at the earliest epochs. | WITSTOK J., JONES G.C., MAIOLINO R., et al. | ||
2023A&A...676A.115P | 19 | D | 1 | 44 | ~ | Unraveling the formation histories of the first supermassive black holes with the Square Kilometre Array's pulsar timing array. | PADMANABHAN H. and LOEB A. | ||
2023ApJ...954L..10F | 280 | X | 6 | 11 | ~ | First Constraints on Dense Molecular Gas at z = 7.5149 from the Quasar Pōniuā'ena. | FERUGLIO C., MAIO U., TRIPODI R., et al. | ||
2023ApJ...954..164T | 19 | D | 2 | 102 | ~ | Modeling the Central Supermassive Black Hole Mass of Quasars via the LSTM Approach. | TABASI S.S., SALMANI R.V., KHALILIYAN P., et al. | ||
2023A&A...678A.201Z | 718 | D | X C | 15 | 20 | ~ | HYPerluminous quasars at the Epoch of ReionizatION (HYPERION): A new regime for the X-ray nuclear properties of the first quasars. | ZAPPACOSTA L., PICONCELLI E., FIORE F., et al. | |
2023A&A...680A..82C | 3079 | A | D | X C | 66 | 4 | ~ | Metal enrichment and evolution in four z > 6.5 quasar sightlines observed with JWST/NIRSpec. | CHRISTENSEN L., JAKOBSEN P., WILLOTT C., et al. |