Accurate Baryon Acoustic Oscillations reconstruction via semi-discrete optimal transport

(2021)

Authors:

Sebastian VON HAUSEGGER, Bruno Lévy, Roya Mohayaee

A geometric distance to the supermassive black Hole of NGC 3783

Astronomy and Astrophysics 654 (2021)

Authors:

A Amorim, M Bauböck, MC Bentz, W Brandner, M Bolzer, Y Clénet, R Davies, PT De Zeeuw, J Dexter, A Drescher, A Eckart, F Eisenhauer, NM Förster Schreiber, PJV Garcia, R Genzel, S Gillessen, D Gratadour, S Hönig, D Kaltenbrunner, M Kishimoto, S Lacour, D Lutz, F Millour, H Netzer, CA Onken, T Ott, T Paumard, K Perraut, G Perrin, PO Petrucci, O Pfuhl, MA Prieto, D Rouan, J Shangguan, T Shimizu, J Stadler, A Sternberg, O Straub, C Straubmeier, R Street, E Sturm, LJ Tacconi, KRW Tristram, P Vermot, S Von Fellenberg, F Widmann, J Woillez

Abstract:

The angular size of the broad line region (BLR) of the nearby active galactic nucleus NGC 3783 has been spatially resolved by recent observations with VLTI/GRAVITY. A reverberation mapping (RM) campaign has also recently obtained high quality light curves and measured the linear size of the BLR in a way that is complementary to the GRAVITY measurement. The size and kinematics of the BLR can be better constrained by a joint analysis that combines both GRAVITY and RM data. This, in turn, allows us to obtain the mass of the supermassive black hole in NGC 3783 with an accuracy that is about a factor of two better than that inferred from GRAVITY data alone. We derive MBH = 2.54-0.72+0.90 × 107 M⊙ . Finally, and perhaps most notably, we are able to measure a geometric distance to NGC 3783 of 39.9-11.9+14.5 Mpc. We are able to test the robustness of the BLR-based geometric distance with measurements based on the Tully-Fisher relation and other indirect methods. We find the geometric distance is consistent with other methods within their scatter. We explore the potential of BLR-based geometric distances to directly constrain the Hubble constant, H0, and identify differential phase uncertainties as the current dominant limitation to the H0 measurement precision for individual sources.

The search for living worlds and the connection to our cosmic origins

Experimental Astronomy Springer 54:2-3 (2021) 1275-1306

Authors:

Ma Barstow, S Aigrain, Jk Barstow, M Barthelemy, B Biller, A Bonanos, L Buchhave, Sl Casewell, C Charbonnel, S Charlot, R Davies, N Devaney, C Evans, M Ferrari, L Fossati, B Gansicke, M Garcia, de Castro AI Gomez, T Henning, C Lintott, C Knigge, C Neiner, L Rossi, C Snodgrass, D Stam, E Tolstoy, M Tosi

Abstract:

One of the most exciting scientific challenges is to detect Earth-like planets in the habitable zones of other stars in the galaxy and search for evidence of life. During the past 20 years the detection of exoplanets, orbiting stars beyond our own, has moved from science fiction to science fact. From the first handful of gas giants, found through radial velocity studies, detection techniques have increased in sensitivity, finding smaller planets and diverse multi-planet systems. Through enhanced ground-based spectroscopic observations, transit detection techniques and the enormous productivity of the Kepler space mission, the number of confirmed planets has increased to more than 2000. Several space missions, including TESS (NASA), now operational, and PLATO (ESA), will extend the parameter space for exoplanet discovery towards the regime of rocky Earth-like planets and take the census of such bodies in the neighbourhood of the Solar System. The ability to observe and characterise dozens of potentially rocky Earth-like planets now lies within the realm of possibility due to rapid advances in key space and imaging technologies and active studies of potential missions have been underway for a number of years. The latest of these is the Large UV Optical IR space telescope (LUVOIR), one of four flagship mission studies commissioned by NASA in support of the 2020 US Decadal Survey. LUVOIR, if selected, will be of interest to a wide scientific community and will be the only telescope capable of searching for and characterizing a sufficient number of exo-Earths to provide a meaningful answer to the question “Are we alone?”. This contribution is a White Paper that has been submitted in response to the ESA Voyage 2050 Call.

Constraining particle acceleration in Sgr A with simultaneous GRAVITY, Spitzer, NuSTAR, and Chandra observations

Astronomy and Astrophysics 654 (2021)

Authors:

R Abuter, A Amorim, M Bauböck, F Baganoff, JP Berger, H Boyce, H Bonnet, W Brandner, Y Clénet, R Davies, PT De Zeeuw, J Dexter, Y Dallilar, A Drescher, A Eckart, F Eisenhauer, GG Fazio, NM Förster Schreiber, K Foster, C Gammie, P Garcia, F Gao, E Gendron, R Genzel, G Ghisellini, S Gillessen, MA Gurwell, M Habibi, D Haggard, C Hailey, FA Harrison, X Haubois, G Heißel, T Henning, S Hippler, JL Hora, M Horrobin, A Jiménez-Rosales, L Jochum, L Jocou, A Kaufer, P Kervella, S Lacour, V Lapeyrère, JB Le Bouquin, P Léna, PJ Lowrance, D Lutz, S Markoff, K Mori, MR Morris, J Neilsen, M Nowak, T Ott, T Paumard, K Perraut, G Perrin, G Ponti, O Pfuhl, S Rabien, G Rodríguez-Coira, J Shangguan, T Shimizu, S Scheithauer, HA Smith, J Stadler, DK Stern, O Straub, C Straubmeier, E Sturm, LJ Tacconi, F Vincent, SD Von Fellenberg, I Waisberg, F Widmann, E Wieprecht, E Wiezorrek, SP Willner, G Witzel, J Woillez, S Yazici, A Young, S Zhang, G Zins

Abstract:

We report the time-resolved spectral analysis of a bright near-infrared and moderate X-ray flare of Sgr A. We obtained light curves in the M, K, and H bands in the mid-and near-infrared and in the 2 -8 keV and 2 -70 keV bands in the X-ray. The observed spectral slope in the near-infrared band is νLν ? ν0.5 ± 0.2; the spectral slope observed in the X-ray band is νLν ? ν-0.7 ± 0.5. Using a fast numerical implementation of a synchrotron sphere with a constant radius, magnetic field, and electron density (i.e., a one-zone model), we tested various synchrotron and synchrotron self-Compton scenarios. The observed near-infrared brightness and X-ray faintness, together with the observed spectral slopes, pose challenges for all models explored. We rule out a scenario in which the near-infrared emission is synchrotron emission and the X-ray emission is synchrotron self-Compton. Two realizations of the one-zone model can explain the observed flare and its temporal correlation: one-zone model in which the near-infrared and X-ray luminosity are produced by synchrotron self-Compton and a model in which the luminosity stems from a cooled synchrotron spectrum. Both models can describe the mean spectral energy distribution (SED) and temporal evolution similarly well. In order to describe the mean SED, both models require specific values of the maximum Lorentz factor γmax, which differ by roughly two orders of magnitude. The synchrotron self-Compton model suggests that electrons are accelerated to γmax ∼ 500, while cooled synchrotron model requires acceleration up to γmax ∼ 5 × 104. The synchrotron self-Compton scenario requires electron densities of 1010 cm-3 that are much larger than typical ambient densities in the accretion flow. Furthermore, it requires a variation of the particle density that is inconsistent with the average mass-flow rate inferred from polarization measurements and can therefore only be realized in an extraordinary accretion event. In contrast, assuming a source size of 1 RS, the cooled synchrotron scenario can be realized with densities and magnetic fields comparable with the ambient accretion flow. For both models, the temporal evolution is regulated through the maximum acceleration factor γmax, implying that sustained particle acceleration is required to explain at least a part of the temporal evolution of the flare.

Inference of the optical depth to reionization from low multipole temperature and polarization Planck data

Monthly Notices of the Royal Astronomical Society 507:1 (2021) 1072-1091

Authors:

R De Belsunce, S Gratton, W Coulton, G Efstathiou

Abstract:

This paper explores methods for constructing low multipole temperature and polarization likelihoods from maps of the cosmic microwave background anisotropies that have complex noise properties and partial sky coverage. We use Planck 2018 High Frequency Instrument (HFI) and updated SRoll2 temperature and polarization maps to test our methods. We present three likelihood approximations based on quadratic cross spectrum estimators: (i) a variant of the simulation-based likelihood (SimBaL) techniques used in the Planck legacy papers to produce a low multipole EE likelihood; (ii) a semi-analytical likelihood approximation (momento) based on the principle of maximum entropy; (iii) a density-estimation 'likelihood-free' scheme (delfi). Approaches (ii) and (iii) can be generalized to produce low multipole joint temperature-polarization (TTTEEE) likelihoods. We present extensive tests of these methods on simulations with realistic correlated noise. We then analyse the Planck data and confirm the robustness of our method and likelihoods on multiple inter- and intra-frequency detector set combinations of SRoll2 maps. The three likelihood techniques give consistent results and support a low value of the optical depth to reoinization, τ, from the HFI. Our best estimate of τ comes from combining the low multipole SRoll2momento (TTTEEE) likelihood with the CamSpec high multipole likelihood and is τ = 0.0627+0.0050-0.0058. This is consistent with the SRoll2 team's determination of τ, though slightly higher by ∼0.5σ, mainly because of our joint treatment of temperature and polarization.